Rollable optical fiber ribbon with low attenuation, large mode field diameter optical fiber and cable

ABSTRACT

A rollable optical fiber ribbon utilizing low attenuation, bend insensitive fibers and cables incorporating such rollable ribbons are provided. The optical fibers are supported by a ribbon body, and the ribbon body is formed from a flexible material such that the optical fibers are reversibly movable from an unrolled position to a rolled position. The optical fibers have a large mode filed diameter, such as ≥9 microns at 1310 nm facilitating low attenuation splicing/connectorization. The optical fibers are also highly bend insensitive, such as having a macrobend loss of ≤0.5 dB/turn at 1550 nm for a mandrel diameter of 15 mm.

PRIORITY APPLICATION

This application is a continuation of U.S. patent application Ser. No.17/742,682, filed May 12, 2022, which continuation of U.S. patentapplication Ser. No. 17/172,579, filed Feb. 10, 2021, now U.S. Pat. No.11,360,280, which is a continuation of U.S. patent application Ser. No.16/853,892, filed Apr. 21, 2020, now U.S. Pat. No. 10,948,674, which isa continuation of U.S. patent application Ser. No. 16/055,773, filedAug. 6, 2018, now U.S. Pat. No. 10,649,163, which claims priority toProvisional Application No. 62/542,480, filed on Aug. 8, 2017, thecontent of each of which is relied upon and incorporated herein byreference in its entirety.

BACKGROUND

The disclosure relates generally to rollable optical fiber ribbons andmore particularly to rollable optical fiber ribbons that utilize lowattenuation, highly bend insensitive fibers with a large mode fielddiameter. The disclosure also relates to densely packed cables utilizingthe low attenuation, rollable fiber optic ribbons discussed herein.Optical cables have seen increased use in a wide variety of fieldsincluding various electronics and telecommunications fields. Opticalcables contain or surround one or more optical fibers. The cableprovides structure and protection for the optical fibers within thecable.

SUMMARY

One embodiment of the disclosure relates to rollable optical fiberribbon. The ribbon includes a plurality of optical fibers. Each opticalfiber includes a mode field diameter of ≥9 microns at 1310 nm and amacrobend loss of ≤0.5 dB/turn at 1550 nm for a mandrel diameter of 15mm. The ribbon includes a ribbon body coupled to and supporting theplurality of optical fibers in an array. The ribbon body is formed froma flexible material such that the plurality of optical fibers arereversibly movable from an unrolled position in which the plurality ofoptical fibers are substantially aligned with each other to a rolledposition.

An additional embodiment of the disclosure relates to an optical cable.The optical cable includes a polymeric outer cable jacket defining anexterior surface of the cable. The optical cable includes a plurality ofoptical fiber ribbons surrounded by the polymeric outer cable jacket.Each of the optical fiber ribbons comprising a plurality of opticalfibers coupled together via a ribbon body, and the ribbon body is formedfrom a flexible material such that the plurality of optical fibers arereversibly movable from an unrolled position to a rolled position. Eachoptical fiber includes a mode field diameter of ≥9 microns at 1310 nmand a macrobend loss of ≤0.5 dB/turn at 1550 nm for a mandrel diameterof 15 mm.

An additional embodiment of the disclosure relates to cable including acable jacket. The cable includes a plurality of buffer tubes surroundedby the cable jacket. The cable includes an optical fiber ribbon locatedwithin each buffer tube. Each optical fiber ribbon includes a pluralityof optical fibers coupled together via a ribbon body. The ribbon body isformed from a flexible material such that the plurality of opticalfibers are reversibly movable from an unrolled position to a rolledposition. The cable includes active particles located within each buffertube, and an average maximum outer dimension of the active particleswithin the buffer tube is ≤50 microns. Each optical fiber includes amode field diameter of ≥9 microns at 1310 nm and a macrobend loss of≤0.5 dB/turn at 1550 nm for a mandrel diameter of 15 mm.

Additional features and advantages will be set forth in the detaileddescription which follows, and in part will be readily apparent to thoseskilled in the art from the description or recognized by practicing theembodiments as described in the written description and claims hereof,as well as the appended drawings.

It is to be understood that both the foregoing general description andthe following detailed description are merely exemplary, and areintended to provide an overview or framework to understand the natureand character of the claims.

The accompanying drawings are included to provide a furtherunderstanding and are incorporated in and constitute a part of thisspecification. The drawings illustrate one or more embodiment(s), andtogether with the description serve to explain principles and operationof the various embodiments.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a cross-sectional view of an optical fiber cable according toan exemplary embodiment.

FIGS. 2A-2C are cross-sectional views of optical fiber buffer tubesaccording to exemplary embodiments.

FIG. 3 is a graph showing the minimum ratio of buffer tube innerdiameter to optical fiber outer diameter as a function of number ofoptical fibers in the buffer tube.

FIG. 4 is a cross-sectional view of an optical fiber cable according toanother exemplary embodiment.

FIG. 5 is a cross-sectional view of an optical fiber cable according toanother exemplary embodiment.

FIG. 6 is a cross-sectional view of an optical fiber cable according toanother exemplary embodiment.

FIG. 7 is a cross-sectional view of an optical fiber cable according toanother exemplary embodiment.

FIG. 8 shows a refractive index profile corresponding to one embodimentof an optical waveguide fiber as disclosed herein.

FIG. 9 shows a refractive index profile of an embodiment of an opticalfiber as disclosed herein.

FIG. 10 shows a refractive index profile of an embodiment of an opticalfiber as disclosed herein.

FIG. 11 shows a refractive index profile of an embodiment of an opticalfiber as disclosed herein.

FIG. 12 shows a refractive index profile of an embodiment of an opticalfiber as disclosed herein.

FIG. 13 shows a refractive index profile of an embodiment of an opticalfiber as disclosed herein.

FIG. 14 shows a refractive index profile of an embodiment of an opticalfiber as disclosed herein.

FIG. 15 shows a cross-sectional view of an optical fiber buffer tubeincluding small sized active particles according to an exemplaryembodiment.

FIG. 16 is a schematic cross-sectional view showing a small sized activeparticle located within a space between optical fibers within the buffertube of FIG. 15 , according to an exemplary embodiment.

FIG. 17 is a graph showing signal attenuation change vs. fiber strainfor various optical cables having different sized SAPparticles/materials, according to an exemplary embodiment.

FIG. 18A is a graph showing signal attenuation during thermal cyclingfor optical fibers within buffer tubes having conventional 75 micron SAPparticles.

FIG. 18B is a graph showing signal attenuation during thermal cyclingfor optical fibers within buffer tubes having small diameter 25 micronSAP particles, according to an exemplary embodiment.

FIG. 19 shows a perspective view of a rollable optical fiber ribbonaccording to an exemplary embodiment.

FIG. 20 shows a cross-sectional view of the optical fiber ribbon of FIG.19 in an unrolled or aligned position according to an exemplaryembodiment.

FIG. 21 shows a cross-sectional view of the optical fiber ribbon of FIG.19 in a rolled or curved position according to an exemplary embodiment.

FIG. 22 shows a perspective view of a rollable optical fiber ribbonaccording to another exemplary embodiment.

FIG. 23 shows a cross-sectional view of a rollable optical fiber ribbonaccording to another exemplary embodiment.

FIG. 24 shows a cross-sectional view of the rollable optical fiberribbon of FIG. 23 in a rolled or curved position according to anexemplary embodiment.

FIG. 25 shows a cross-sectional view of the rollable optical fiberribbon of FIG. 23 in another rolled or curved position according to anexemplary embodiment.

FIG. 26 shows a cross-sectional view of a rollable optical fiber ribbonaccording to another exemplary embodiment.

FIG. 27 shows a cross-sectional view of a rollable optical fiber ribbonaccording to another exemplary embodiment.

FIG. 28 shows a cross-sectional view of a rollable optical fiber ribbonaccording to another exemplary embodiment.

FIG. 29 shows a cross-sectional view of a rollable optical fiber ribbonin a rolled or curved position according to another exemplaryembodiment.

FIG. 30 shows a cross-sectional view of a rollable optical fiber ribbonin a rolled or curved position according to another exemplaryembodiment.

FIG. 31 shows a cross-sectional view of a rollable optical fiber ribbonin a rolled or curved position located within a buffer tube according toanother exemplary embodiment.

FIG. 32 shows a cross-sectional view of a rollable optical fiber ribbonin a rolled or curved position located within a buffer tube according toanother exemplary embodiment.

FIG. 33 shows a system configured to form a rollable optical fiberribbon according to an exemplary embodiment.

FIG. 34 is a cross-sectional view of cable including rollable opticalfiber ribbons according to an exemplary embodiment.

FIG. 35 is a cross-sectional view of cable including rollable opticalfiber ribbons located within a cable jacket without buffer tubesaccording to an exemplary embodiment.

DETAILED DESCRIPTION

Referring generally to the figures, various embodiments of a rollableoptical fiber ribbon utilizing low attenuation, bend insensitive fibersand of cables incorporating such rollable ribbons are shown. Asbackground, some optical fiber cables are deployed or used in ways thatmay induce bend losses in optical signals transmitted through theoptical fibers of the cable. Such bend losses can be caused by cabledeployments that include tight bend radii, compression of optical fiber,etc., that induce bend losses. Further, such bend losses can beexperienced in a wide variety of cables, such optical drop cableassemblies, distribution cables with Factory Installed TerminationSystems (FITS) and slack loops.

In addition, bend losses may be greater in cables in which opticalfibers are densely packed in relatively rigid buffer tubes, are denselypacked within a cable jacket and/or are densely packed in an opticalfiber ribbon arrangement. Bend losses in such cables are caused, atleast in part, by positional constraint resulting from the dense packingwhich limits the ability of optical fibers to shift to assume low strainpositions during bending, compression, etc. Such bend losses inconventional cables may be further increased when optical fibers aresupported by a flexible ribbon matrix and then rolled, for example intoa curved cross-sectional shape. Thus, typical optical fiber cable and/orbuffer tube configurations include a significant amount of free-spacebetween the outer surfaces of the optical fibers and the inner surfaceof the buffer tube or jacket, and this free-space allows the opticalfibers to move or shift to assume low stress positions during bending.By reducing stress that the optical fibers experience during bending,such low density cables provide a satisfactory level of signalattenuation, but do so with a relatively large diameter buffer tubeand/or relatively large cable jacket.

In particular embodiments discussed herein, Applicant has developed newrollable fiber optic ribbons that utilize low attenuation, highly bendinsensitive optical fibers. As discussed in detail herein, these highlybend insensitive optical fibers allow for a variety of unique and highlydesirable optical cable designs utilizing a rollable fiber optic ribbon.Providing a rollable optical fiber ribbon as discussed herein mayprovide a number of benefits as compared to conventional optical fiberribbons or conventional loose buffered optical fibers includingincreased fiber count, higher packing density, easier connectorization,higher transmission rates, decreased ribbon size and may eliminate theneed for buffer tubes, in at least some applications.

As one example of an advantage of the rollable ribbon designs discussedherein, furcation of standard ribbon cable designs requiresstripping/removing/severing of a standard ribbon matrix at the furcationpoint, allowing the fibers of the ribbon to be routed from the maincable body and through a small cylindrical furcation tube. At the end ofthe furcation tube, the optical fibers need to be realigned (typicallyby hand) and held in a linear array via application of a glue-likematerial to allow for splicing of the optical fibers to an opticalconnector (e.g., via mass fusion splicing). This labor intensive stepcan be improved by providing a fiber optic cable with a rollable ribbonsupporting the optical fibers. The rollable ribbon can assume a rolledshape that can be passed into the furcation tube without removal of theribbon matrix, and at the end of the furcation tube, the rollable ribbonis simply unrolled to a linear arrangement suitable for splicing to theconnector. Thus, the time consuming steps of stripping the ribbon matrixand the manual realignment of optical fibers for coupling to the opticalconnector are avoided via the designs discussed herein.

Further, in the past, rollable ribbon designs have encountereddifficulties related to high bend loss attenuation and attenuation atthe connection to the optical connector. To address these deficiencies,the rollable optical fiber ribbon discussed herein utilizes highly bendinsensitive fibers having a significantly improved mode field diameter(MFD) as compared to prior bend insensitive fibers. As such, therollable ribbons discussed herein provide the handling and organizationadvantages of the rollable ribbon design while providing an MFD whichallows for very low levels of signal loss at the optical connector.Thus, the rollable ribbons discussed herein provide the benefit of easyhandling and connectorization without the connector attenuationtypically caused by the relatively low MFD of typical bend insensitivefibers that has plagued prior attempts to utilize prior bend insensitivefibers in rollable ribbon designs.

Further, in addition to having much improved MFD, the bend insensitivefibers discussed herein have very low macro and/or micro bendattenuation characteristics that allow for tightly rolled optical fiberribbons that can be densely packed within a cable while still providingfor acceptable bend attenuation, despite the tight roll and/or densepacking of the ribbon. In specific embodiments, the designs discussedherein allow for very high fiber count optical cables (e.g., cableshaving at least 432 optical fibers, at least 1728 optical fibers, atleast 3456 optical fibers, etc.) that also have relatively low outercable diameters. In such embodiments, these optical cables deliver ahigh fiber count, small size along with the handling advantages of arollable ribbon, while maintaining the bend attenuation and large modefield diameter (≥9 microns at 1310 nm) for low coupling losses and easyalignment when spliced or connected to itself and/or standard SMFfibers. Due to the need to balance a wide variety of design parameterswhen designing an optical cable (e.g., cable size, fiber count, bendattenuation, connector attenuation, ribbon handling/organizationlimitations, etc.), Applicant believes a rollable ribbon that includesthe highly bend insensitive optical fibers discussed herein achieves acombination of cable performance unachievable in the past.

Overview of Rollable Ribbon with Bend Insensitive Fiber and RelatedCables

As will generally be understood, optical cables utilizing a rollableribbon have design and function at the fiber design level, at the ribbondesign level and at the cable design level. For clarity, thisapplication describes each of these design levels and relatedembodiments in the separate sections outlined below, and this overviewsection provides a brief introduction to the technology described indetail within this application.

Referring generally to FIGS. 19-35 and to the associated description,various embodiments of rollable optical ribbons and related disclosureare provided. In general, the ribbon embodiments disclosed herein areconfigured to allow the ribbon to be bent, curved or rolled from anunrolled position to a rolled or curved position. In such embodiments,optical fibers are coupled to and supported by a ribbon body. The ribbonbody is formed from a material that is configured to allow the ribbon tobe rolled and unrolled as needed.

The ribbon embodiments discussed herein may utilize a ribbon matrix thatcompletely or partially surrounds the optical fibers when viewed inlongitudinal cross-section. Generally, the ribbon body is formed from amaterial, such as a polymer material, that has an elasticity and/orthickness that allows for the rollability of the ribbon. In someembodiments, the ribbon body may be formed from a plurality of discretesections or bridges spaced along the longitudinal axis of adjacentoptical fibers. In other various embodiments, the ribbon body iscontiguous, both lengthwise and widthwise, over the optical fibers.

Referring to FIGS. 8-14 and to the associated description, details ofbend insensitive fibers, and particularly bend insensitive fibers havinga large MFD that facilitates low signal loss connectorization areprovided. In specific embodiments, as discussed in more detail below,the rolled ribbon designs discussed herein utilize optical fibers havingMFD≥9 microns at 1310 nm, opticals compatible with ITU G.652 and G.657Astandards and/or macrobend loss at 15 mm bend mandrel diameter of ≤0.5dB/turn. The rollable ribbon designs utilizing the bend insensitive,G.652 and G.657A compatible fibers disclosed herein allows for cableswith high fiber density that have low coupling losses when connected tostandard SMF fibers and that also have low bend loss attenuation and theorganizational/handling advantages of an optical fiber ribbon.

In various embodiments, the optical fibers disclosed herein arecompatible with G.652 standards, have macrobend loss at 15 mm mandreldiameter of ≤0.5 dB/turn and a zero dispersion wavelength between 1300nm and 1324 nm. In various embodiments, these optical fibers include alower index trench region in the cladding layer, that helps to reducebend loss. In various embodiments, the volume of the trench region islarger than 30% Δ micron². In some embodiments, the volume of the trenchregion is larger than 50% Δ micron². In other embodiments, the volume ofthe trench region is larger than 70% Δ micron². In still otherembodiments, the volume of the trench region is larger than 90% Δmicron². Some of the optical fiber designs have a core alpha ≤5, and insuch designs, the lower index trench region in the cladding is adjacentto the fiber core. Some of the optical fiber designs have core alphabetween 10 and 100, and in such embodiments, the lower index trenchregion in the cladding is offset from the fiber core by an innercladding layer. In some embodiments the coating diameter of the fiber is≤250 microns, in other embodiments the coating diameter of the fiber is≤210 microns, and in still other embodiments the coating diameter of thefiber is ≤190 microns.

In various embodiments, the combination of the highly bend insensitiveoptical fibers and the rollable ribbon designs discussed herein allowfor densely packed and/or high fiber count optical fiber cables thatalso allow for easy handling, connectorization, furcation andorganization provided by the use rollable ribbon designs. Referring toFIGS. 1-7 and to the associated description, details of various denselypacked optical cable designs are provided. In various embodiments, thecables discussed herein include at least 432 optical fibers. In variousembodiments, the cables discussed herein include at least 864 opticalfibers. In various embodiments, the cables discussed herein include atleast 1728 optical fibers. In yet other embodiments, the cablesdiscussed herein include at least 3456 optical fibers.

In addition, referring to FIGS. 15-18B and to the associateddescription, the rollable optical fiber ribbons discussed herein may beutilized within optical cables utilizing small sized/diameterparticulate material (e.g., small diameter water blocking powder). Asdiscussed in detail below, Applicant has found that use of smallparticles within a fiber optic cable reduces micro-bend attenuation, andthus, utilization of these small particles in combination with therollable ribbons discussed herein further improves overall cableattenuation performance.

High Density Cable Designs

Referring to FIG. 1 , an optical cable, shown as cable 10, isillustrated according to an exemplary embodiment. Cable 10 includes anouter cable jacket, shown as outer jacket 12, having an inner surface 14that defines an inner passage or cavity, shown as central bore 16, andan outer surface 18 that generally defines the outermost surface ofcable 10. As will be generally understood, inner surface 14 of jacket 12defines an internal area or region within which the various cablecomponents discussed herein are located.

In various embodiments, cable jacket 12 is formed from an extrudedthermoplastic material. In various embodiments, cable jacket 12 may be avariety of materials used in cable manufacturing such as polyethylene,medium density polyethylene, polyvinyl chloride (PVC), polyvinylidenedifluoride (PVDF), nylon, polyester or polycarbonate and theircopolymers. In addition, the material of cable jacket 12 may includesmall quantities of other materials or fillers that provide differentproperties to the material of cable jacket 12. For example, the materialof cable jacket 12 may include materials that provide for coloring,UV/light blocking (e.g., carbon black), burn resistance, etc.

Cable 10 includes one or more optical transmission elements or opticalwaveguides, shown as optical fibers 20. In the embodiment shown, groupsof optical fibers 20 are located in separate buffer tubes 22, and buffertubes 22 are wrapped (e.g., in an SZ stranding pattern) around a centralstrength member 24. In various embodiments, optical fibers 20 aresupported by a rollable ribbon body or ribbon matrix as discussedherein. In various embodiments, cable 10 includes at least four buffertubes 22. Central strength member 24 may be any suitable axial strengthmember, such as a glass-reinforced plastic rod, steel rod/wire, etc.Generally, cable 10 provides structure and protection to optical fibers20 during and after installation (e.g., protection during handling,protection from elements, protection from the environment, protectionfrom vermin, etc.).

In various embodiments, cable 10 also includes an armor layer, shown asarmor 26. In general, armor 26 is formed from a strip of metal material(e.g., a metal tape, a flat elongate continuous piece of material, etc.)that is wrapped around and circumferentially surrounds buffer tubes 22.As shown in FIG. 1 , armor 26 is located adjacent to the inner surfaceof outer jacket 12 such that these two layers are in contact with eachother. In specific embodiments, armor 26 is corrugated steel tapematerial that is wrapped around the interior portions of cable 10, andin some such embodiments, armor 26 is longitudinally folded forming alongitudinal overlapped section where opposing edges of the tape overlapto completely surround inner buffer tubes 22 (and any other interiorcomponent of cable 10). In other embodiments, armor 26 may be a strip ofmetal tape material, helically wrapped around buffer tubes 22 such thatarmor 26 forms a layer circumferentially surrounding buffer tubes 22. Ingeneral, armor layer 26 provides an additional layer of protection tofibers 20 within cable 10, and may provide resistance against damage(e.g., damage caused by contact or compression during installation,damage from the elements, damage from rodents, etc.). Cable 10 mayinclude a variety of other components or layers, such as helicallywrapped binders, circumferential constrictive thin-film binders, waterblocking tape materials, water-blocking fiber materials, etc. As definedherein the minimum cable core diameter is the minimum diameter withoutstranding of the buffer tube bundle surrounding and the central member.In some embodiments, stranding the buffer tubes will increase thediameter of the cable core by 1 to 15 percent. In some embodiments,stranding the buffer tubes will increase the diameter of the cable coreby 1 to 5 percent.

In the embodiment shown, cable 10 includes one or more preferential tearfeature and/or ripcord 28 embedded in or underneath jacket 12. In thisembodiment, preferential tear feature and/or ripcord 28 is located withjacket 12 such that ripcord 28 facilitates opening of outer jacket 12.In some embodiments, ripcord 28 may be located within armor layer 26such that ripcord 28 facilitates opening of both armor 26 and jacket 12.

In various embodiments cable 10, optical fibers 20 and buffer tube 22are configured in various ways to provide a high fiber density, highfiber count cable while at the same time reducing or minimizing buffertube size and/or cable jacket size. As discussed herein, low diameteroptical fibers allows higher density and smaller cable, and the low bendloss design of these optical fibers allows such high density and smallcable to have acceptable signal loss properties. In embodiments whereoptical fibers 20 are supported by a rollable ribbon body, cable 10 isprovided with the organizational and handling advantages of a ribbonwhile still allowing for dense packing.

Referring to FIGS. 2A-2C, various buffer tube designs having differentlevels of fiber packing density are shown. FIGS. 2A-2C show threedifferent buffer tube designs, shown as buffer tubes 22′, 22″ and 22′.In general, buffer tubes 22′, 22″ and 22′″ are polymeric tubes thatsurround, protect and organize optical fibers 20, and further buffertubes 22′, 22″ and 22′″ are generally the same as each other except forthe buffer tube's inner diameter and the resulting optical fiber packingarrangement within each buffer tube discussed in more detail below.Further, it should be understood that cable 10 may include buffer tubes22′, 22″ and/or 22′″ in any combination. In various embodiments, cable10 includes only one of buffer tubes types 22′, 22″ or 22″, and in otherembodiments, cable 10 includes a mixture of buffer tubes 22′, 22″ and/or22′″.

Referring to FIG. 2A, buffer tube 22′ includes a buffer tube wall 30having an inner surface 32 and an outer surface 34. Inner surface 32defines a buffer tube channel 36 within which optical fibers 20 arelocated. As shown in FIG. 2A, optical fibers 20 are arranged into anouter group 38 and an inner group 40 within channel 36. Generally, theoptical fibers 20 of outer group 38 are located in the outer portion ofchannel 36 adjacent to (e.g., <5 microns from) or in contact with innersurface 32 such that outer group 38 surrounds inner group 40. Innergroup 40 is generally located in a central region of channel 36.

Inner surface 32 defines a buffer tube inner diameter D1, and in thespecific embodiment shown in FIG. 2A, D1 is sized such that opticalfibers 20 have full positional constraint. In the specific embodimentshown in FIG. 2A, the inner diameter of buffer tube 22′ is smallrelative to the outer fiber diameter, D2, and the number of fibers, N,which results in the full positional constraint shown in FIG. 2A. Inparticular, buffer tube 22′ is sized such that a maximum gap length,shown as G, measured between any pair of adjacent optical fibers 20 ofouter group 38 is less than an outer diameter, D2, of one or moreoptical fiber 20 of inner group 40 such that optical fibers 20 of theinner group 40 are blocked from moving from the inner group 40 to theouter group 38. Thus, in this manner buffer tube 22′ results in a fullypositionally constrained fiber arrangement, and in this arrangement,buffer tube 22′ provides a densely packed unit of optical fibers.Specifically, the portion of the area of channel 36 occupied by opticalfibers 20 is high, and the overall inner diameter D1 is low resulting inbuffer tube with a large fiber count in a relatively small area.

In particular embodiments, Applicant has determined a relationshipbetween D1 and D2 that defines dense packing of optical fibers 20 withinbuffer tube 22′ as provided by the present disclosure. As a specificexample, in various embodiments discussed herein, optical fibers 20 aredensely packed within buffer tube 22′ such that a diameter ratioparameter, Ω (Omega), which is defined as the ratio, D1/D2, is less than2.66+0.134(N), where N is the number of optical fibers 20 within buffertube 22′, and in addition, in a specific embodiment, Ω is also greaterthan 2.25+0.143(N), where N is the number of optical fibers 20 withinbuffer tube 22′. In various embodiments, N is at least 4, specifically Nis greater than 6, and more specifically N is 8 to 24, inclusive of 8and 24. In another embodiment, N is 12 to 24, inclusive of 12 and 24. Inanother embodiment, N is greater than 24, and in one such embodiment,8≤N≤48. In the specific embodiment shown in FIG. 2A, N is 12, D1 isgreater than or equal to 4.030 times the fiber OD and less than or equalto 4.273 times the fiber OD. In addition, in this 12 fiber embodiment,outer group 38 has 9 optical fibers 20 and inner group 40 has 3 opticalfibers 20.

In various embodiments, the degree of packing of optical fibers 20within tube 22′ can be understood as the ratio of the minimum diameter,D4, of a circle circumscribing all fibers 20 of outer group 38, tobuffer tube inner diameter D1. In the embodiments shown in FIGS. 2A-2C,D4 is relatively large such that more than half, and specifically allfibers 20 of outer group 38 are in contact with inner surface 32. Invarious embodiments, fibers 20 are packed such that the ratio D4/D1 isgreater than 0.95, specifically is greater than 0.97, more specificallygreater than 0.99 and even more specifically greater than 0.995. Invarious cable embodiments utilizing these densely packed buffer tubes,Applicant believes that the interaction between the outer surfaces offibers 20 and the inner surface 32 of tube wall 30 may increase tensilestrength of the cable constructed from such tubes, and in suchembodiments, the utilization of the various bend insensitive fibersdiscussed herein provides for satisfactory optical attenuation despitethe high level of fiber/tube interaction.

Referring to FIGS. 2B and 2C, different levels of fiber packing densityand positional constraint are shown. FIG. 2B shows a buffer tube 22″sized to provide partial positional constraint to optical fiber 20movement within buffer tube 22″, according to an exemplary embodiment.As shown in FIG. 2B, inner diameter D1 of buffer tube 22″ is sized suchthat one of the optical fibers 20 of inner group 40 just fits in the gap42 between a pair of adjacent optical fibers 20 of outer group 38 andcan move back into the inner group 40. As a comparison, FIG. 2C showsbuffer tube 22′″ sized to provide no positional constraint on opticalfibers 20 within buffer tube 22′.

In various embodiments, buffer tubes 22 of cable 10 as discussed hereinhave at least some positional constraint. As a specific example, invarious embodiments discussed herein, optical fibers 20 are denselypacked within a buffer tube, such as buffer tube 22′ of 22″, such that adiameter ratio parameter, Q, which is defined as the ratio, D1/D2, isless than 1.14+0.313(N), where N is the number of optical fibers 20within buffer tube 22′ or 22″, and in addition, in a specificembodiment, Q is also greater than 2.25+0.143(N), where N is the numberof optical fibers 20 within buffer tube 22′ and 22″. In variousembodiments, N is at least 4, specifically N is greater than 6, and morespecifically N is 8 to 24, inclusive of 8 and 24. In another embodiment,N is 12 to 24, inclusive of 12 and 24. In another embodiment, N isgreater than 24, and in one such embodiment, 8≤N≤48. In the specificembodiment shown in FIG. 2B, N is 12, D1 of buffer tube 22″ is greaterthan or equal to 4.273 times the fiber OD and less than or equal to 4.87times the fiber OD and specifically less than 4.864 times the fiber OD.In addition, in this 12 fiber embodiment of buffer tube 22″, outer group38 has 9 optical fibers 20, and inner group 40 has 3 optical fibers 20,and one optical fiber 20 of inner group 40 is permitted to movepartially into gap 42 as shown in FIG. 2B.

As a comparison, FIG. 2C, shows buffer tube 22′ sized to have nopositional constraint such that one or more optical fibers 20 arepermitted to move freely between inner group 40 and outer group 38,which allows optical fibers 20 to assume low strain positions duringbending, but requires a larger inner diameter D1 and less dense packingas compared to buffer tubes 22′ and 22″. Specifically, as shown in FIG.2C, optical fibers 20 are not densely packed within buffer tube 22′″such that a diameter ratio parameter, Ω, of buffer tube 22′″ which isdefined as the ratio, D1/D2, is greater than 1.14+0.313(N), where N isthe number of optical fibers 20 within buffer tube 22′, for, N greater6, N greater than 24, and N 8 to 24, inclusive of 8 and 24. In thespecific embodiment shown in FIG. 2C, N is 12, D1 of buffer tube 22′″ isgreater than or equal to 4.864 times the fiber OD.

In specific embodiments, the dense fiber packing and high fiber countwithin buffer tube 22′ is facilitated by an optical fiber having a lowouter diameter, and various optical fiber properties that allows for lowsignal loss despite the dense packing and high fiber count. In variousembodiments, such fibers may have a variety of properties in variouscombinations, such as an outer diameter D2≤210 microns, a mode fielddiameter of ≥9 microns at 1310 nm, a cable cutoff of ≤1260 nm, amacrobend loss of ≤0.5 dB/turn at 1550 nm for a mandrel diameter of 15mm, and/or a wire-mesh covered drum microbending loss at 1550 nm of≤0.03 dB/km. In some such embodiments, D2 is ≤190 microns. In otherembodiments, such fibers may have a variety of properties in variouscombinations, such as an outer diameter D2≤210 microns, a mode fielddiameter of ≥9 microns at 1310 nm, a cable cutoff of ≤1260 nm, amacrobend loss of ≤0.5 dB/turn at 1550 nm for a mandrel diameter of 20mm, and/or a wire-mesh covered drum microbending loss at 1550 nm of≤0.03 dB/km. In some such embodiments, D2 is ≤190 microns. In specificembodiments, optical fibers 20 may be any of the optical fibers orinclude any of the optical fiber features or characteristics discussedherein. It should be understood that the outer fiber diameters discussedherein, such as D2, are the outer diameter measured at the outer surfaceof the outermost polymer fiber coating layer, typically a secondarypolymer coating as discussed herein.

In various embodiments, tube walls 30 of buffer tubes 22′, 22″ and 22′″are relatively rigid, relatively thick polymer structures such thatduring bending, tube walls 30 do not deform to a sufficient degree toallow for optical fibers 20 to assume a low strain position throughdeformation of the buffer tube wall itself. This is in contrast to someoptical fiber bundles or micromodules that are densely packed byutilizing flexible, thin bundle jackets. In such optical fiber bundlesdense packing and acceptable bend loss characteristics are achievedthrough the flexible nature of the bundle jacket which allows for fibermovement during bending. In contrast to such optical fiber bundles, invarious embodiments, buffer tubes 22′ and 22″ do not allow forsubstantial movement and achieves acceptable bend loss characteristicsvia use of low diameter, bend insensitive optical fibers, such as thosediscussed herein.

In various embodiments, tube walls 30 have a thickness T1 that isbetween 50 microns and 250 microns. In particular embodiments, tubewalls 30 are formed from a material having a having a modulus ofelasticity at 25° C. between 0.8 GPa and 3 GPa. In various embodimentsdiscussed herein, tube walls 30 having these thicknesses and/or moduliform relatively rigid tubular structures that do not bend, stretch,deform, etc. to a significant amount within the cable, and thus, in suchembodiments, optical fibers 20 are bend insensitive fibers as discussedherein. Such bend insensitive fibers allow for low optical attenuationdespite residing in highly packed, thick and/or high modulus tubes 22.

Buffer tube walls 30 may be made from a variety of suitable polymermaterials. In one embodiment, buffer tube walls 30 are formed from apolypropylene material. In another embodiment, buffer tube walls 30 areformed from a polycarbonate material. In various embodiments, buffertube walls 30 are formed from one or more polymer material includingpolybutylene terephthalate (PBT), polyamide (PA), polyoxymethylene(POM), polyvinylchloride (PVC), flame retardant PCV, poly(ethylene-co-tetrafluoroethene) (ETFE), or various combinations of thepolymer materials discussed herein, etc. In various embodiments, thematerial of buffer tube walls 30 may include various fillers oradditives including UV blocking materials and burn resistant materials.

As a specific example of the various buffer tube sizing and fiberpacking of the present disclosure, FIG. 3 shows a plot of the minimumratio of buffer tube inner diameter to fiber outer diameter as afunction of the number of fibers in the buffer tube. Plot 50 shows thenormalized effective bundle diameter assumed for a defined number offibers in a bundle and plot 52 shows the minimum normalized tube ID tojust accommodate a defined number of fibers. This is a fit to themodeled data defining the minimum normalized diameter of circumscribingcircle to just fit around each bundle of fibers from 1 to 48 fibers.

Referring back to FIG. 1 , in particular embodiments, one or more buffertubes 22 of cable 10 is one or more of densely packed buffer tube, suchas buffer tubes 22′ and 22″ discussed above. In such embodiments, thedense packing and small diameter of buffer tubes 22′ or 22″ allow forcable 10 to also be densely packed and have a small diameter despitehaving a large number of optical fibers 20. As shown in FIG. 1 , cable10 has an outer diameter, D3, that is less than 15 mm, and in theparticular embodiment shown, cable 10 has this low outer diameter whileincluding at least 72 optical fibers located in 6 buffer tubes.

Referring to FIG. 4 , an optical fiber cable 60 is shown according to anexemplary embodiment. Cable 60 is substantially the same as cable 10except as discussed herein. As shown, cable 60 includes at least 144optical fibers, and includes at least 12 buffer tubes 22 each including12 optical fibers 20. Like cable 10, cable 60 includes an outer diameterD3 that is less than 15 mm, and buffer tubes 22 are fully constrainedbuffer tubes 22′. In other embodiments, buffer tubes 22 of cable 60 maybe buffer tubes 22″ and/or buffer tubes 22′″. In addition, cable 10includes a jacketed central strength member 62 including central portion64 and an outer jacket 66. In particular embodiments, central portion 64may be relatively rigid, such as a metal material or glass reinforcedplastic, and outer jacket 66 is a polymer coating.

Referring to FIG. 5 , an optical fiber cable 70 is shown according to anexemplary embodiment. Cable 70 is substantially the same as cable 10except as discussed herein. As shown, cable 70 includes at least 96optical fibers, and includes at least 8 buffer tubes 22 each including12 optical fibers 20. Like cable 10, cable 70 includes an outer diameterD3 that is less than 15 mm, and buffer tubes 22 are fully constrainedbuffer tubes 22′. In other embodiments, buffer tubes 22 of cable 70 maybe buffer tubes 22″ and/or buffer tubes 22′″.

Referring to FIG. 6 , an optical fiber cable 80 is shown according to anexemplary embodiment. Cable 80 is substantially the same as cable 10except as discussed herein. As shown cable 80 includes at least 72optical fibers, and includes at least 6 buffer tubes 22 each including12 optical fibers 20. In the specific embodiment shown, buffer tubes 22are unconstrained buffer tubes 22′″. Thus, cable 80 achieves very lowbend loss through use of both unconstrained buffer tubes 22′″ whichallows for fibers 20 to move during bending to achieve low strainpositions in combination with the low diameter, low bend loss opticalfibers discussed herein.

Referring to FIG. 7 , an optical fiber cable 90 is shown according to anexemplary embodiment. Cable 90 is substantially the same as cable 10except as discussed herein. As shown cable 90 includes a single buffertube 92, and a stack 94 of a plurality of optical fiber ribbons 96. Eachoptical fiber ribbon 96 includes a plurality of optical fibers 20surrounded by and supported by a polymeric matrix 98. In variousembodiments, cable 90 includes at least four ribbons within stack 94 andeach ribbon 96 supports four optical fibers 20. In some embodiments,like cable 10, cable 90 includes an outer diameter D3 that is less than15 mm. In such embodiments cable 90 provides a low bend loss, lowdiameter ribbon cable utilizing the low diameter, low bend loss opticalfibers discussed herein. In various embodiments, ribbons 96 are rollableribbons and matrix 98 is formed from a flexible material that permitsrolling of ribbons 96 as discussed herein.

Low Bend Loss, Large Mode Field Diameter Optical Fibers

Optical fibers 20 discussed herein are configured to experience lowsignal loss during bending. In various embodiments, optical fibers 20discussed herein may be any of the optical fibers discussed herein andspecifically may be configured as the various embodiments of opticalfiber 110, discussed herein. In addition, in various embodiments,optical fibers 216 discussed below in relation to specific rollableribbon designs may be any of the optical fibers discussed herein andspecifically may be configured as the various embodiments of opticalfiber 110, discussed herein.

According to at least some embodiments the optical fibers have lowbend-induced losses especially for tight bends, such as 15 mm diameterbends, for applications in data centers and fiber to the homeinstallations. According to at least some embodiments the optical fibersdisclosed herein are backward compatible with existing installed fibernetwork systems. According to at least some embodiments, the opticalfibers disclosed herein have a 1310 nm wavelength mode field diameter of≥8.6 microns in order to have low splice losses with existing installedoptical fibers. According to at least some embodiments, the opticalfibers disclosed herein have a 1310 nm wavelength mode field diameterof >9 microns in order to have low splice losses with existing installedoptical fibers. Optical fibers disclosed herein can be cabled and can bepart of a network system having a transmitter and receiver.

The “refractive index profile” is the relationship between refractiveindex or relative refractive index and the fiber radius. The radius foreach segment of the refractive index profile is given by theabbreviations r₁, r₂, r₃, r_(4a), r₄, etc. and lower an upper case areused interchangeability herein (e.g., r₁ is equivalent to R₁).

The “relative refractive index percent” (also referred to herein as“refractive index delta percent”, “relative refractive index”,“refractive index delta”, and “relative refractive index delta”) isdefined as Δ%=100×(n_(i) ²−n_(c) ²)/2n_(i) ², and as used herein n_(c)is the average refractive index of undoped silica. As used herein, therelative refractive index is represented by Δ and its values are givenin units of “%”, unless otherwise specified. The terms: delta, Δ, Δ%, %Δ, delta %, % delta and percent delta may be used interchangeablyherein. For embodiments described herein, an equivalent relativerefractive index profile can be obtained by shifting the entirerefractive index profile of the optical fiber is either up or down. Incases where the refractive index of a region is less than the averagerefractive index of undoped silica, the relative refractive indexpercent is negative and is referred to as having a depressed region ordepressed index. In cases where the refractive index of a region isgreater than the average refractive index of the cladding region, therelative refractive index percent is positive. An “updopant” is hereinconsidered to be a dopant which has a propensity to raise the refractiveindex relative to pure undoped SiO₂. A “downdopant” is herein consideredto be a dopant which has a propensity to lower the refractive indexrelative to pure undoped SiO₂. Examples of updopants include GeO₂(germania), Al₂O₃, P₂O₅, TiO₂, Cl, Br. Examples of down dopants includefluorine and boron.

“Chromatic dispersion”, herein referred to as “dispersion” unlessotherwise noted, of a waveguide fiber is the sum of the materialdispersion, the waveguide dispersion, and the inter-modal dispersion. Inthe case of single mode waveguide fibers the inter-modal dispersion iszero. Zero dispersion wavelength is a wavelength at which the dispersionhas a value of zero. Dispersion slope is the rate of change ofdispersion with respect to wavelength.

“Effective area” is defined as in equation 1 as:A _(eff)=2π(˜f ² rdr)²/(˜f ⁴ rdr)  Eq. 1where the integration limits are 0 to ∞, r is the radial distance fromthe center of the core, and f is the transverse component of theelectric field associated with light propagated in the waveguide. Asused herein, “effective area” or “A_(eff)” refers to optical effectivearea at a wavelength of 1550 nm unless otherwise noted.

The term “α-profile” refers to a refractive index profile, expressed interms of Δ(r) which is in units of “%”, where r is radius, which followsthe equation 2, shown belowΔ(r)=Δ(r _(o))(1−[|r−r _(o)|/(r ₁ −r _(o))]^(α))  Eq. 2where r_(o) is the point (radial location) in the core at which Δ(r) ismaximum, r₁ is the point at which Δ(r) % is zero, and r is in the ranger_(i)≤r≤r_(f), where Δ is defined above, r_(i), is the initial point ofthe α-profile, r_(f) is the final point of the α-profile, and α is anexponent which is a real number (referred to as “core α”, “core alpha”,“alpha value” or “α value” herein).

The mode field diameter (MFD) is measured using the Peterman II methodwherein, 2w=MFD, and w²=(2˜f²rdr/˜[df/dr]²rdr), the integral limitsbeing 0 to ∞.

The bend resistance of a waveguide fiber can be gauged by inducedattenuation under prescribed test conditions, for example by deployingor wrapping the fiber around a mandrel of a prescribed diameter, e.g.,by wrapping 1 turn around a either a 6 mm, 10 mm, or 20 mm or similardiameter mandrel (e.g. “1×10 mm diameter macrobend loss” or the “1×20 mmdiameter macrobend loss”) and measuring the increase in attenuation perturn.

One type of bend test is the lateral load microbend test. In thisso-called “lateral load” test (LLWM), a prescribed length of waveguidefiber is placed between two flat plates. A #70 wire mesh is attached toone of the plates. A known length of waveguide fiber is sandwichedbetween the plates and a reference attenuation is measured while theplates are pressed together with a force of 30 Newtons. A 70 Newtonforce is then applied to the plates and the increase in attenuation indB/m is measured. The increase in attenuation is the lateral loadattenuation of the waveguide in dB/m at a specified wavelength(typically within the range of 1200-1700 nm, e.g., 1310 nm or 1550 nm or1625 nm).

Another type of bend test is the wire mesh covered drum microbend test(WMCD). In this test, a 400 mm diameter aluminum drum is wrapped withwire mesh. The mesh is wrapped tightly without stretching, and shouldhave no holes, dips, or damage. Wire mesh material specification:McMaster-Carr Supply Company (Cleveland, Ohio), part number 85385T106,corrosion-resistant type 304 stainless steel woven wire cloth, mesh perlinear inch: 165×165, wire diameter: 0.0019″, width opening: 0.0041″,open area %: 44.0. A prescribed length (750 meters) of waveguide fiberis wound at 1 m/s on the wire mesh drum at 0.050 centimeter take-uppitch while applying 80 (+/−1) grams tension. The ends of the prescribedlength of fiber are taped to maintain tension and there are no fibercrossovers. The attenuation of the optical fiber is measured at aspecified wavelength (typically within the range of 1200-1700 nm, e.g.,1310 nm or 1550 nm or 1625 nm); a reference attenuation is measured onthe optical fiber wound on a smooth drum. The increase in attenuation isthe wire mesh covered drum attenuation of the waveguide in dB/km at aspecified wavelength (typically within the range of 1200-1700 nm, e.g.,1310 nm or 1550 nm or 1625 nm).

Another type of bend test is the basketweave microbend loss test. In thebasketweave microbend loss test, the fibers are wound at high tension ona glass spool and exposed to a temperature cycle. The testing apparatuscomprises of a fixed diameter silica drum. The drum surface is smooth.In this test, the drum diameter is 110 mm. The fiber is wound onto theglass drum with a winding tension of 70 grams, and a pitch of 2 mm(distance between adjacent wraps of fiber). Multiple layers of fiber arewrapped with this tension and pitch. The pitch angles are reversed witheach layer wound. The crossover of the tensioned fibers from theadjacent layers creates the microbend mechanism. A fiber length of 2.5km is used. The initial fiber attenuation measurement is performed atabout 23°, at about 45% RH (relative humidity) with the fiber deployedin the basketweave configuration with 70 grams of tension. Initialattenuation loss measurements are made at wavelengths of 1310 nm, 1550nm, and 1625 nm. An OTDR (optical time domain reflectometer) is used toacquire the attenuation loss data.

After the initial attenuation loss measurement at 23° C., the fiber issubjected to thermal cycling. In the thermal cycling, the fiber is firstcooled from 23° C. to −60° C. at a rate of 1° C./min. The fiber ismaintained at −60° C. for 20 hours and then heated at a rate of 1°C./min back to 23° C. The fiber is maintained at 23° C. for 2 hours,then heated to 70° C. at a rate of 1° C./min and maintained at 70° C.for 20 hours. The fiber is then cooled to 23° C. at a rate of 1° C./minand maintained at 23° C. for two hours. The fiber is then subjected to asecond thermal cycle, which was identical to the first thermalcycle—i.e., it is cooled from 23° C. to −60° C., then heated back to 23°C., maintained at that temperature for 2 hours and then heated from 23°C. to 70° C., after which it is cooled back to 23° C. Finally, aftermaintaining the fiber at a temperature of 23° C. for two hours, afterthe second cycle, the fiber is once again cooled to −60° C. at a rate of1° C./min, held at −60° C. for 20 hours, and then further cooled at arate of 1° C./min to −60° C. The fiber is held at −60° C. for 20 hours,then heated at a rate of 1° C./min back to 23° C. and held at 23° C. for2 hours. The thermal cycling is concluded at this point.

During the thermal cycling of the fiber, the attenuation loss of thefiber is measured continuously. The maximum attenuation loss over thetwo thermal cycles down to −60° C. is determined, and the differencebetween this maximum attenuation loss and the initial attenuation lossat 23° C. is reported herein, as the basketweave microbend loss of thefiber over the temperature range from −60° C. to 70° C. In the thermalcycle down to −60° C., the difference between the attenuation lossmeasured at −60° C. and the initial attenuation loss at 23° C. isreported herein as the basketweave microbend loss of the fiber over thetemperature range from −60° C. to 23° C.

The “pin array” bend test is used to compare relative resistance ofwaveguide fiber to bending. To perform this test, attenuation loss ismeasured for a waveguide fiber with essentially no induced bending loss.The waveguide fiber is then woven about the pin array and attenuationagain measured. The loss induced by bending is the difference betweenthe two measured attenuations. The pin array is a set of ten cylindricalpins arranged in a single row and held in a fixed vertical position on aflat surface. The pin spacing is 5 mm, center to center. The pindiameter is 0.67 mm. During testing, sufficient tension is applied tomake the waveguide fiber conform to a portion of the pin surface. Theincrease in attenuation is the pin array attenuation in dB of thewaveguide at a specified wavelength (typically within the range of1200-1700 nm, e.g., 1310 nm or 1550 nm or 1625 nm).

The theoretical fiber cutoff wavelength, or “theoretical fiber cutoff”,or “theoretical cutoff”, for a given mode, is the wavelength above whichguided light cannot propagate in that mode. A mathematical definitioncan be found in Single Mode Fiber Optics, Jeunhomme, pp. 39-44, MarcelDekker, New York, 1990 wherein the theoretical fiber cutoff is describedas the wavelength at which the mode propagation constant becomes equalto the plane wave propagation constant in the outer cladding. Thistheoretical wavelength is appropriate for an infinitely long, perfectlystraight fiber that has no diameter variations.

Fiber cutoff is measured by the standard 2 m fiber cutoff test, FOTP-80(EIA-TIA-455-80), to yield the “fiber cutoff wavelength”, also known asthe “2 m fiber cutoff” or “measured cutoff”. The FOTP-80 standard testis performed to either strip out the higher order modes using acontrolled amount of bending, or to normalize the spectral response ofthe fiber to that of a multimode fiber.

By cabled cutoff wavelength, “cable cutoff”, “cable cutoff wavelength”,or “cabled cutoff” as used herein, we mean the cable cutoff wavelengthdetermined by the 22 m cabled cutoff test described in the EIA-445 FiberOptic Test Procedures, which are part of the EIA-TIA Fiber OpticsStandards, that is, the Electronics Industry Alliance—TelecommunicationsIndustry Association Fiber Optics Standards,

Unless otherwise noted herein, optical properties (such as dispersion,dispersion slope, etc.) are reported for the LP01 mode.

Optical fibers disclosed herein are capable of exhibiting an effectivearea at 1550 nm which is greater than about 70 microns², in someembodiments between 75 and 95 microns², for example between about 80 and90 microns². In some embodiments, the optical mode effective area at1550 nm is between about 82 and 88 microns².

The embodiments of the fiber 110 is (see, for example, FIG. 8 ) includea core 112 with comprising maximum refractive index delta percent Δ₁ anda cladding 120 that surrounds the core 112. In at least some embodimentsdisclosed herein the core alpha is larger than 5 (i.e., α>5). Accordingto the exemplary embodiments described herein, fiber 110 is preferably asingle mode fiber.

The cladding 120 includes inner cladding region 121 that is in contactwith and surrounds the core 112, a depressed index cladding region 122(also referred to as a trench region herein) that surrounds the innercladding region 121. The cladding region 122 has a refractive indexdelta percent 43. The outer cladding region 124 surrounds the trenchregion 122 and comprises a refractive index delta percent 44. A trenchregion is a low refractive index region, surrounded by the higherrefractive index regions. As shown for example, in FIG. 8 , the trenchregion 122 within the cladding 120 is surrounded by two higher indexcladding regions—i.e., cladding regions 121 and 124.

In the embodiments described herein Δ_(1max)>Δ₄; Δ₃<Δ₂; and Δ₄>Δ₃. Inthe embodiments illustrated in FIGS. 8-14 , cladding regions 121, 122and 124 are immediately adjacent one another. However, this is notrequired, and alternatively, additional cladding regions may beemployed.

The core 112 comprises an outer radius r₁ (which is defined as where atangent line drawn through maximum slope of the refractive index deltapercent of central core 112 crosses the zero delta line) that is between2.75 and 6 microns, in some embodiments between about 3 and 5.75microns, for example between 3.5 and 5.6 microns, and in someembodiments 4-5 microns. Core 112 exhibits a refractive index deltapercent Δ₁, (relative to pure silica). For example the maximumrefractive index delta of the core, Δ_(1max), may be 0 percent (if it ismade of pure silica) to 0.65 percent, or between 0.15 and 0.5 percent,and in some embodiments between about 0.2 and 0.5 percent. In someembodiments Δ_(1max)≥0.38, for example 0.5≥Δ_(1max)≥0.38.

In some embodiments, the core 112 exhibits a core alpha (α) wherein, αis greater than 5, for example at least 10. In some embodiments the corealpha is 15 or greater. In some embodiments, the core 112 may comprisean alpha between about 10 and 100, for example in some embodiments thecore alpha, α, may be between 15 and 100, and in some embodimentsbetween 15 and 40. A refractive index profile of an exemplary fiberembodiment with α₁ of about 20 is shown, for example, in FIG. 8 .

In the embodiments illustrated in FIG. 10-14 , the inner cladding region121 is adjacent to the core 112 and comprises inner radius r₁ and outerradius r₂. The inner cladding region 121 preferably exhibits arefractive index delta percent, Δ₂≤0.3 (relative to pure silica). Asstated above, Δ₁≥Δ₂. In the exemplary embodiments described herein,0.15%≤Δ_(1max)−Δ₂≤0.5%, for example 0.2%<Δ_(1max)−Δ₂<0.4%, or0.25%<Δ_(1max)−Δ₂<0.35. In some embodiments Δ₂ is 0 to 0.3 percent, forexample between about 0 and 0.25 percent, or between 0.1 and 0.2percent. Alternatively, for example, if the core region 112 (alsoreferred to as a core herein) is made of pure silica, the inner claddingregion 121 is downdoped relative to pure silica, such thatΔ_(1max)−Δ₂≤0.5 percent. The outer radius r₂ of the inner claddingregion 121 is between 5 and 17 microns, in some embodiments betweenabout 7 and 15 microns, for example 6 to 12 microns, or 6 to 10 microns.In some embodiments the ratio of r₂/r₁ is >1.2. In some embodiments theratio of r₂/r₁ is ≥1.25, for example 1.25≤r₂/r₁≤2.5. In at least some ofthe exemplary embodiments described herein 1.6≤r₂/r₁≤2.4. In at leastsome of the exemplary embodiments described herein 1.8≤r₂/r₁≤2.35. Theabove values of the radius r₁, the difference between Δ_(1max) and Δ₂,and the r₂/r₁ ratio help the fibers have 1300 nm≤λ₀≤1324 nm and MFDbetween 8.2 microns and 9.5 microns at the 1310 nm wavelength.

The trench region 122 (also referred to as depressed index claddingregion herein) surrounds the inner cladding region 121. The trenchregion 122 has a refractive index delta percent Δ₃ that is smaller thanΔ₂. In some embodiments Δ₃ is −0.4%≤Δ₃≤0.1%. For example, in someembodiments the trench is formed of pure silica, and Δ₃ is 0. In someembodiments the relative refractive index delta percent in the trenchregion 122 is essentially flat, i.e. the difference between the relativerefractive index delta percent at any two radii within the trench region122 is less than 0.03%, and in some embodiments less than 0.01%. Inother embodiments there can be fluctuations as a result of small profiledesign or process variations. In some embodiments, the trench region 122comprises silica which is substantially undoped with either fluorine orgermania, i.e., such that the region is essentially free of fluorine andgermania, i.e., less than 0.1 wt. % F or GeO₂. In some embodiments, thetrench region is pure silica, in other embodiments it is silica dopedwith fluorine, in order to make −0.4%≤Δ₃≤0.1%. In some embodiments,0.35%≤Δ_(1max)−Δ₃≤0.65%.

The trench region 122 preferably exhibits a width W_(t) (whereinW_(t)=r₃−r₂) between about 4 microns and 22 microns, in someembodiments, between 8 and 20 microns. In some embodiments, the outerradius r₃ of the trench region may be not less than 10 microns, forexample greater than 12 microns and less than 27 microns, or about 14.5microns to about 25.5 microns in order to achieve good bend performanceand a cable cutoff of ≤1260 nm.

Outer cladding region 124 surrounds the trench region 122 and comprisesrefractive index delta percent Δ₄ which is higher than the refractiveindex delta percent Δ₃ of the trench region 122, thereby forming aregion which is an “updoped” outer cladding region 124 with respect tothe depressed index cladding region 122, e.g., by adding an amount ofdopant (such as germania or chlorine) sufficient to increase therefractive index of the outer cladding region. In some embodiments,there is no fluorine or other down dopants in the trench region 122, andthe outer cladding region 124 comprises an updopant, for examplechlorine. In some embodiments, the chlorine concentration in the outercladding region 124 is ≥1 wt. %. In some other embodiments, the chlorineconcentration in the outer cladding region 124 is ≥1.2 wt. %. In stillother embodiments, the chlorine concentration in the outer claddingregion 124 is ≥1.5 wt. %. In yet other embodiments, the chlorineconcentration in the outer cladding region 124 is ≥2 wt. %.

Outer cladding region 124 comprises a higher refractive index than thatof the trench region 122, and may, for example, have a refractive indexdelta percent Δ₄ which is between 0.12% and 0.4%. In some embodiments0.12%≤Δ₄−Δ₃≤0.4%, for example in some embodiments 0.12%<Δ₄−Δ₃<0.3%. Insome embodiments, the outer cladding region 124 is comprised of a firstouter cladding region 123 (with an outer radius r_(4a)) and a secondouter cladding region 125 (with an outer radius r₄), wherein the firstouter cladding region 123 has a chlorine concentration of ≥1.2 wt % fromr₃ to 40 microns. In some embodiments first outer cladding region 123has a chlorine concentration of ≥1.5 wt. % from r₃ to 40 microns, and insome embodiments, the first outer cladding region 123 has a chlorineconcentration of ≥2 wt. % from r₃ to 40 microns.

In some embodiments, the second outer cladding region 125 has a higherviscosity than the first outer cladding layer. That is, the viscosity ofthe glass of the second outer cladding region 125 is greater than theviscosity of glass of the first outer cladding region 123. In thisembodiment the second outer cladding region 125 is the tension absorbinglayer. In some embodiments, the second outer cladding region 125 has achlorine concentration of ≤0.5 wt. % from r_(4a) to r₄ (where r_(4a) isthe outer radius of the high (e.g., ≥1.2 wt. % Cl) updoped region, asshown for example in FIG. 9 , and r₄ is the outer radius of the glassoptical fiber, for example, 62.5 microns). In some embodiments thesecond outer cladding region 125 has a chlorine concentration of ≤0.25wt. % from its inner radius r_(4a) to the outer radius r₄. In someembodiments the second outer cladding region has a chlorineconcentration, [Cl], of 0.0 wt. % [Cl]≤0.2 wt. % from r_(4a) to r₄. Insome embodiments, 40 microns ≤r_(4a)≤55 microns, for example r_(4a) isat 40 microns, 45 microns, 50 microns, or 55 microns. Preferably, thehigher index portion (compared trench region 122) of outer claddingregion 124 extends at least to the point where the optical power whichwould be transmitted through the optical fiber is greater than or equalto 90% of the optical power transmitted, more preferably to the pointwhere the optical power which would be transmitted through the opticalfiber is greater than or equal to 95% of the optical power transmitted,and most preferably to the point where the optical power which would betransmitted through the optical fiber is greater than or equal to 98% ofthe optical power transmitted, which is preferred to achieve good bendperformance and a cable cutoff of ≤1260 nm. In some embodiments, this isachieved by having the “updoped” third annular region (i.e., the firstouter cladding region 123) extend at least to a radial point of about 30microns. In some embodiments, the “updoped” third annular region 123extends at least to a radial point of about 40 microns, with a fourthannular region (i.e., the second outer cladding region 125) comprisingessentially of silica surrounding the third annular region. In someembodiments, the cladding 120 has an outer diameter of 2 times themaximum radius, R_(max), of about 125 micron. As shown in FIG. 9 , theupdoped region 123 (i.e., the first outer cladding region) of the outercladding 124, has a refractive index delta percent of Δ₄ and thecladding region 125 (i.e., the second outer cladding region) has arefractive index delta percent of Δ₅, and Δ₄>Δ₅.

The profile volume V₃ of the trench region 122, is calculated usingΔ₍₄₋₃₎(r)rdr between radius r₂ and r₃, and thus is defined in equation 3as

$\begin{matrix}{V_{3} = {2{\int\limits_{r2}^{r3}{{\Delta_{({4 - 3})}(r)}{rdr}}}}} & {{Eq}.3}\end{matrix}$

All volumes are in absolute magnitude (i.e., V3=|V₃|). In order toachieve good bend performance, the volume V₃ of the trench region 122 ispreferably greater than 30% Δmicron², and may be greater than 45%Δmicron², and in some embodiments is greater than 50% Δmicron², and insome embodiments may be greater than 55% Δmicron². In some embodimentsthe volume V₃ of the trench region 122 is 30% Δ micron² to 90% Δmicron², for example 40 to 80% Δ micron².

In the exemplary embodiments disclosed herein the core 112 has apositive refractive index throughout. The core region 112 comprises amaximum refractive index delta percent Δ_(1 max) occurring between r=0and r=3 microns. In these embodiments Δ_(1 max) is between about 0.38%and about 0.5%.

The fibers are capable of exhibiting a bend loss of ≤0.5 dB/turn whenwound upon on a 15 mm diameter mandrel for fibers with MAC numbers≥7.25. In some embodiments, the optical fibers disclosed herein have aMAC number of ≥7.6 or even ≥7.7 and in some examples, 7.6≤MAC ≤8, and azero dispersion wavelength, λ₀ of 1324 nm≥λ₀≥1300 nm. As used herein,MAC number means mode field diameter at 1310 (nm) divided by 22 m cablecutoff wavelength (nm).

The fibers disclosed herein may be drawn from optical fiber preformsmade using conventional manufacturing techniques and using known fiberdraw methods and apparatus, for example as is disclosed in U.S. Pat.Nos. 7,565,820, 5,410,567, 7,832,675, 6,027,062, the specifications ofwhich are hereby incorporated by reference.

Various exemplary embodiments will be further clarified by the followingexamples. It will be apparent to those skilled in the art that variousmodifications and variations can be made without departing from thespirit or scope of the claims.

Optical Fiber Examples

Table 1 below lists characteristics of fiber embodiments examples 1-3.These fiber embodiments have refractive index profiles as shown in FIGS.10-12 . In particular, set forth below for each example is therefractive index delta percent Δ₁, alpha 1 (α1), and outer radius r₁ ofthe core 112; refractive index delta percent Δ₂, and outer radius r₂ ofthe inner cladding region 121; and refractive index delta percent Δ₃,and outer radius r₃, as well as profile volume V₃ of the trench region122, which is calculated between r₂ and r₃; refractive index deltapercent Δ₄. Also set forth are chromatic dispersion and dispersion slopeat 1310 nm, chromatic dispersion and dispersion slope at 1550 nm, modefield diameter at 1310 nm and 1550 nm, lateral load wire mesh microbendat 1550 nm, pin array macrobend at 1550 nm, zero dispersion wavelength(Lambda 0), 22 m cable cutoff, MAC number at 1310 nm, 1×15 mm diameterbend loss (bend loss when the fiber is turned once around a 15 mmdiameter mandrel), and spectral attenuation at 1310 and 1550 nm.

TABLE 1 Parameter Ex 1 Ex 2 Ex 3 Δ1max (%) 0.47 0.47 0.45 r₁ (micron)4.3 4.3 4.3 Region12 20 20 20 Core Alpha Δ2 (%) 0.15 0.15 0.15 Δ1-Δ20.32 0.32 0.30 r₂ (micron) 10 9 8.1 r₂/r₁ 2.3 2.1 1.9 Δ3 (%) 0.00 0.000.00 Δ2-Δ3 0.15 0.15 0.15 r₃(micron) 20 19.5 20 Δ4 (%) 0.15 0.15 0.15r₄(micron) 62.5 62.5 62.5 Max chlorine 1.5 1.5 1.5 concentration inouter cladding region 124, weight % Δ4-Δ3 0.15 0.15 0.15 V3 45 45 50 (%micron²) Dispersion at 4.9E−04 0.346 0.25 1310 nm (ps/nm/km) Dispersion0.088 0.099 0.091 Slope at 1310 nm (ps/nm²/km) Lambda 1318 1315 1315zero, nm Dispersion at 17.5 18 18 1550 nm (ps/nm/km) Dispersion at 0.0620.062 0.063 Slope 1550 nm (ps/nm{circumflex over ( )}2/km) MFD at 13109.2 9.16 9.25 nm (micron) MFD at 1550 10.44 10.34 10.38 nm (micron) LLWM@ 0.6 0.56 0.77 1550 nm, dB/m WMCD at 0.04 0.04 0.04 1550 nm, dB/km PinArray at 14.9 15.0 23.9 1550 nm, dB Cable Cutoff 1206 1206 1200 (nm)Aeff at 1310 66.5 65.9 67.2 nm (micron²) Aeff at 1550 85.6 84.0 84.6 nm(micron²) MAC # (MFD 7.63 7.60 7.71 at 1310 nm/Cable Cutoff) 1 × 15 mm0.19 0.2 0.29 diameter bend loss at 1550 nm (dB/turn) 1 × 20 mm 0.0470.047 0.074 diameter bend loss at 1550 nm (dB/turn) 1 × 30 mm 0.00450.0045 0.01 diameter bend loss at 1550 nm (dB/turn) Attn at 1550 0.180.18 0.18 nm, dB/km Attn at 1310 0.32 0.32 0.32 nm, dB/km

As can be seen in Table 1 above, the exemplary fibers shown in Table 1employ a glass core region 112 having index Δ₁, an inner cladding region121 having index Δ₂, and cladding trench region 122 having refractiveindex delta percent Δ₃, and an outer cladding region 124 havingrefractive index delta percent Δ₄; wherein Δ_(1max)>Δ₂; Δ_(1max)>Δ₄;Δ₃>Δ₂; Δ₄>Δ₃, wherein the difference between Δ_(1max) and Δ₂ is greaterthan or equal to at least 0.15, difference between Δ_(1max) and Δ₃ isgreater than or equal to at least 0.35 (e.g., 0.38≤Δ_(1max)−Δ₃≤0.65);the difference between Δ₂ and Δ₃ is greater than or equal to at least0.08 (e.g., 0.08≤Δ₂−Δ₂≤0.4); and the difference between Δ₄ and Δ₃ isgreater than or equal to at least 0.08 (e.g., 0.1≤Δ₄−Δ₃≤0.4, or0.1≤Δ₄−Δ₃≤0.3); and the absolute value of profile volume, |V₃| is atleast 30% micron². These fibers have mode field diameters (MFD) at 1310nm between 9 microns and 9.5 micron, for example between 9.2 microns and9.5 microns and a zero dispersion wavelength between 1300 nm and 1324nm.

Table 2 below lists characteristics of a fiber example 4 embodiment.This fiber embodiments has the refractive index profile as shown in FIG.13 .

TABLE 2 Parameter Ex 4 Δ1max (%) 0.53 r₁ (micron) 4.4 Region12 CoreAlpha 20 Δ2 (%) 0.2 Δ1-Δ2 0.33 r₂ (micron) 10 r₂/r₁ 2.27 Δ3 (%) 0.00Δ2-Δ3 0.2 r₃(micron) 18.2 Δ4 (%) 0.2 r_(4a)(micron) 45 Max chlorineconcentration. in 2 outer cladding region 124, weight % Δ4-Δ3 0.2 Δ5 (%)0 r₄(micron) 62.5 V3 (%micron2) 46.2 Dispersion at 1310 nm 0.483(ps/nm/km) Dispersion Slope at 1310 nm 0.089 (ps/nm²/km) Lambda zero, nm1312 Dispersion at 1550 nm 18.1 (ps/nm/km) Dispersion at Slope 1550 nm0.062 (ps/nm²/km) MFD at 1310 nm (micron) 9.16 MFD at 1550 nm (micron)10.31 LLWM @ 1550 nm, dB/m 0.4 WMCD at 1550 nm, dB/km 0.04 Pin Array at1550 nm, dB 8.96 Cable Cutoff (nm) 1257 Aeff at 1310 nm (micron²) 66.1Aeff at 1550 nm (micron²) 81.7 MAC # (MFD at 1310 7.29 nm/Cable Cutoff)1 × 15 mm diameter bend loss 0.102 at 1550 nm (dB/turn) 1 × 20 mmdiameter bend loss 0.023 at 1550 nm (dB/turn) 1 × 30 mm diameter bendloss 0.002 at 1550 nm (dB/turn) Attn at 1550 nm, dB/km 0.18 Attn at 1310nm, dB/km 0.32

As can be seen in Table 2 above, the exemplary fibers such as thatdepicted in FIG. 9 and FIG. 13 employ a glass core region 112 havingrefractive index delta percent Δ_(1max), an inner cladding region 121having refractive index delta percent Δ₂, and trench region 122 havingrefractive index delta percent Δ₃, and an first outer cladding region123 having refractive index delta percent Δ₄ and a second outer claddingregion 125 having a refractive index delta percent Δ₅; whereinΔ_(1max)>→₂; Δ_(1max)>Δ₄; Δ₃>Δ₂; Δ₄>Δ₃, wherein the difference betweenΔ_(1max) and Δ₂ is greater than or equal to at least 0.15, differencebetween Δ_(1max) and Δ₃ is greater than or equal to at least 0.35 (e.g.,0.38≤Δ_(1max)−Δ₃≤0.65); the difference between Δ₂ and Δ₃ is greater thanor equal to at least 0.08 (e.g., 0.08≤Δ₂−Δ₂≤0.4); and the differencebetween Δ₄ and Δ₃ is greater than or equal to at least 0.08 (e.g.,0.1≤Δ₄−Δ₃≤0.4, or 0.1≤Δ₄−Δ₃≤0.3); and an absolute value of profilevolume, |V₃| of at least 30% micron². In this embodiment, the claddingregion 125 is a silica layer with a relative refractive index percent ofabout zero. The cladding region 125 (i.e., the second outer claddingregion) acts as a stiff tension absorbing layer. This fiber embodimenthas a mode field diameter (MFD) at 1310 nm between 9 microns and 9.5micron, and a zero dispersion wavelength between 1300 nm and 1324 nm.

The fiber embodiments described herein exhibit a cable cutoff less thanor equal to 1260 nm and a bend loss of ≤0.5 dB/turn when wound upon on a15 mm diameter mandrel. These fibers also exhibit a mode field diameterbetween about 9 and 9.5 microns at 1310 nm, a zero dispersion wavelengthbetween 1300 and 1324 nm, a dispersion slope at 1310 nm which is lessthan or equal to 0.092 ps/nm²/km. These fibers exhibit a Wire MeshCovered Drum (WMCD) bend loss at 1550 nm which is less than or equal to0.07 dB/km, in some embodiments less than or equal to 0.06 dB/km, and insome embodiments less than or equal to 0.05 dB/km. These fibers alsoexhibit a pin array bend loss at 1550 nm which is less than 8.5 dB, insome embodiments less than 5 dB and in some embodiments less than 4 dB.These fibers exhibit a Basketweave microbend loss at 1550 nm which isless than or equal to 0.05 dB/km, in some embodiments less than or equalto 0.025 dB/km, and in some embodiments less than or equal to 0.01dB/km.

Many of these fibers also exhibit a bend loss at 1550 nm, when woundupon on a 15 mm diameter mandrel, of ≤0.5 dB/turn, and in some cases≤0.2 dB/turn. These fibers also exhibit a bend loss at 1550 nm, whenwound upon on a 20 mm diameter mandrel, of ≤0.2 dB/turn, in someembodiments ≤0.15 dB/turn, and some fibers in some embodiments ≤0.1dB/turn. These fibers also exhibit a bend loss at 1550 nm, when woundupon on a 30 mm diameter mandrel, of ≤0.02 dB/turn, for example ≤0.005dB/turn, or even ≤0.003 dB/turn.

Such bend loss and attenuation performance numbers are attainable usinga primary and secondary coating applied to the fiber, wherein theYoung's modulus of the primary is less than 2 MPa, in some embodiments≤1 MPa, and in some embodiments ≤0.5 MPa. The Young's modulus of thesecondary coating is greater than 500 MPa, in some embodiments greaterthan 1000 MPa, and in some embodiments greater than 1500 MPa. In someembodiments, the outer diameter of the secondary coating is 242 microns.In some other embodiments, the outer diameter of the secondary coatingis 200 microns.

Table 3 provides data of a manufactured optical fiber embodiment(Example 5 fiber). The refractive index profile of optical fiber example5 fiber is illustrated in FIG. 14 .

TABLE 3 Data for manufactured optical fiber Parameter Ex 5 Δ_(1max) (%)0.48 r₁ (microns) 4.87 Core Alpha, α 20 r₂ (microns) 6.11 r₂/r₁ 1.25Δ2(%) 0.153 R₃ (microns) 19.8 Δ₃ (%) 0 V₃(% Δ micron²) 60 Δ₄ (%) 0.168Chlorine conc. in outer cladding 1.7 region 124, weight % r₄ (microns)62.5 Dispersion at 1310 nm 0.565 (ps/nm/km) Dispersion Slope at 1310 nm0.091 (ps/nm²/km) Dispersion at 1550 nm 18.1 (ps/nm/km) Zero DispersionWavelength (nm) 1304 MFD at 1310 nm (microns) 9.34 MFD at 1550 nm(microns) 10.45 Aeff at 1550 nm (micron²) 85.8 Cable Cutoff (nm) 1204Macrobend Loss for 15 mm 0.078 mandrel diameter at 1550 nm (dB/turn)Macrobend Loss for 20 mm 0.084 mandrel diameter at 1550 nm (dB/turn)Macrobend Loss for 30 mm 0.005 mandrel diameter at 1550 nm (dB/turn)Microbend loss at 1550 nm in 0.005 Basket-weave test at −60 C. for 242microns coating diameter (dB/km) Microbend loss at 1550 nm in 0.03Basket-weave test at −60 C. for 200 microns coating diameter (dB/km)Microbend loss at 1550 nm in 0.03 Basket-weave test at −60 C. for 200microns coating diameter (dB/km)

In the embodiment of Table 3, the optical fibers exhibits a basketweavemicrobend loss at −60° C. at 1550 nm which is less than or equal to 0.05dB/km, for example less than or equal to 0.03 dB/km.

In some embodiments, the fiber core may comprise a relative refractiveindex profile having a so-called centerline dip which may occur as aresult of one or more optical fiber manufacturing techniques. However,the centerline dip in any of the refractive index profiles disclosedherein is optional.

The optical fiber disclosed herein comprises a core 112 and a cladding120 surrounding and directly adjacent to the core. According to someembodiments, the core is comprised of silica doped with germanium, i.e.germania doped silica. Dopants other than germanium, singly or incombination, may be employed within the core, and particularly at ornear the centerline, of the optical fiber disclosed herein to obtain thedesired refractive index and density. In embodiments, the core region112 of the optical fiber 110 disclosed herein has a non-negativerefractive index profile, more preferably a positive refractive indexprofile, with the inner cladding region 121 surrounding and directlyadjacent to core region 112.

In various embodiments discussed herein, the optical fibers include oneor more protective layer (e.g., polymer layers) located outside of andsurrounding outer cladding region 124, and in at least some embodiments,these protective layers are configured to provide puncture resistance tothe optical fiber. For example, the optical fiber disclosed herein maybe surrounded by a protective coating, e.g. a primary coating Pcontacting and surrounding the outer cladding region 124. In variousembodiments, the primary coating P has a Young's modulus of ≤1.0 MPa, insome embodiments, ≤0.9 MPa, and in some embodiments not more than 0.8MPa. In various embodiments, the optical fibers discussed herein furtherincludes a secondary coating S contacting and surrounding the primarycoating P. In various embodiments, the secondary coating S has a Young'smodulus of greater than 1200 MPa, and in some embodiments greater than1400 MPa. In some embodiments, optical fibers discussed herein include aprimary coating P have intrinsic modulus of elasticity ≤0.5 MPa,specifically ≤0.2 MPa and even more preferably ≤0.15 MPa, while glasstransition temperature is between −25 and −35 degrees C., and in somesuch embodiments, the diameter of the primary coating is preferably ≤165um, specifically ≤160 um and even more specifically ≤150 um, and in suchembodiments, the secondary coating diameter is ≤250 microns and morespecifically is ≤210 microns. In various embodiments, the secondarycoating has a modulus of elasticity larger than 1200 MPa, specificallylarger than 1500 MPa and more specifically larger than 1800 MPa. Inparticular embodiments, reduced diameter optical fibers discussed hereinhave secondary coatings with modulus of elasticity of larger than 1700MPa have a puncture resistance load of larger than 25 g, as shown inTable 4 below. The test method for the puncture resistance of theoptical fiber coating can be found in 52^(nd) IWCS (International Wireand Cable Symposium) Proceedings, p. 237-245.

TABLE 4 Puncture resistance testing for reduced diameter optical fibersSecondary coating cross- Minimal puncture Fiber sectional area, microns²load, grams 1  9450 28.0 2 10912 26.8 3 11306 28.2

According to some embodiments, with primary and secondary coatings, theouter diameter of the secondary coating is ≤250 microns. According tosome embodiments the fiber further is coated with primary and secondarycoatings, and the outer diameter of the secondary coating is ≤210microns. According to some embodiments the fiber further is coated withprimary and secondary coatings, and the outer diameter of the secondarycoating is ≤190 microns.

As used herein, the Young's modulus, elongation to break, and tensilestrength of a cured polymeric material of a primary coating is measuredusing a tensile testing instrument (e.g., a Sintech MTS Tensile Tester,or an INSTRON Universal Material Test System) on a sample of a materialshaped as a film between about 0.003″ (76 micron) and 0.004″ (102micron) in thickness and about 1.3 cm in width, with a gauge length of5.1 cm, and a test speed of 2.5 cm/min.

Additional description of suitable primary and secondary coatings can befound in PCT Publication WO2005/010589 which is incorporated herein byreference in its entirety.

Preferably, the optical fibers disclosed herein have a low OH content,and preferably have an attenuation curve which exhibits a relativelylow, or no, water peak in a particular wavelength region, especially inthe E-band. The optical fiber disclosed herein preferably has an opticalattenuation (spectral) at 1383 nm which is not more than 0.10 dB/kmabove an optical attenuation at 1310 nm, and more preferably not morethan the optical attenuation at 1310 nm. The optical fiber disclosedherein preferably has a maximum hydrogen induced attenuation change of<0.03 dB/km at 1383 nm after being subjected to a hydrogen atmosphere,for example 0.01 atm partial pressure hydrogen for at least 144 hours.

A low water peak generally provides lower attenuation losses,particularly for transmission signals between about 1340 nm and about1470 nm. Furthermore, a low water peak also affords improved pumpefficiency of a pump light emitting device which is optically coupled tothe optical fiber, such as a Raman pump or Raman amplifier which mayoperate at one or more pump wavelengths. Preferably, a Raman amplifierpumps at one or more wavelengths which are about 100 nm lower than anydesired operating wavelength or wavelength region. For example, anoptical fiber carrying an operating signal at wavelength of around 1550nm may be pumped with a Raman amplifier at a pump wavelength of around1450 nm. Thus, the lower fiber attenuation in the wavelength region fromabout 1400 nm to about 1500 nm would tend to decrease the pumpattenuation and increase the pump efficiency, e.g. gain per mW of pumppower, especially for pump wavelengths around 1400 nm.

The fibers disclosed herein exhibit low PMD values particularly whenfabricated with OVD processes. Spinning of the optical fiber may alsolower PMD values for the fiber disclosed herein.

High Density Cable Examples

Table 5 shows modeled results for optical fiber cable designs havingfibers disclosed herein. Shown in the table below, these exemplaryembodiments include buffer tube diameter, buffer tube wall thickness,number of optical fibers in each buffer tube, the diameter of theoptical fiber including the coating and coloring layers, the overallnumber of optical fibers in the cable, the number of buffer tubes in thecable, the central member minimum diameter (including the strengthelements and upjacketing), the minimum cable core diameter, the fiberdensity in the cable core and the Q parameter (fiber diameter/insidediameter of the buffer tube). Optical fiber cables in these examples caninclude stranding of the buffer tubes, stranding binder yarns and/orthin film binder to hold the buffer tubes, additional strength membersoutside the cable core, armor, and cable jacketing.

TABLE 5 Optical Fiber Cables Example Example Example Example ExampleExample Example Parameter 1 2 3 4 5 6 7 Buffer Tube Inside 0.92 0.770.89 0.89 0.84 0.84 0.84 Diameter, mm Buffer Tube 0.15 0.15 0.15 0.150.15 0.10 0.05 Thickness, mm Number of Fibers in 8 8 12 12 12 12 12buffer Tube Coated + Colored 0.25 0.21 0.21 0.21 0.21 0.21 0.21 FiberDiameter, mm Overall fiber count in 96 96 72 144 144 144 144 CableBuffer tubes in cable 12 12 6 12 12 12 12 Min central member 3.48 3.061.19 3.41 3.28 2.99 2.71 diameter, mm Min Cable Core 5.92 5.20 3.57 5.795.56 5.07 4.59 Diameter, mm Fiber density in Cable 3.49 4.51 7.19 5.475.93 7.12 8.72 Core (N/mm²) Omega 3.68 3.67 4.24 4.24 4.00 4.00 4.00Example Example Example Example Example Example Example Parameter 8 9 1011 12 13 14 Buffer Tube Inside 1.20 1.22 1.22 0.99 0.87 1.22 1.22Diameter, mm Buffer Tube 0.15 0.15 0.10 0.10 0.15 0.15 0.15 Thickness,mm Number of Fibers in 24 24 24 24 24 24 24 buffer Tube Coated + Colored0.21 0.21 0.21 0.17 0.15 0.21 0.21 Fiber Diameter, mm Overall fibercount in 144 144 144 144 144 288 288 Cable Buffer tubes in cable 6 6 6 66 12 12 Min central member 1.50 1.53 1.43 1.19 0.88 4.37 4.37 diameter,mm Min Cable Core 4.50 4.57 4.27 3.57 3.22 7.41 7.41 Diameter, mm Fiberdensity in Cable 9.05 8.77 10.04 14.36 17.64 6.67 6.67 Core (N/mm²)Omega 5.71 5.81 5.81 5.82 5.80 5.81 5.81

The cable examples in Table 5 show cables comprising buffer tube innerdiameters between 0.75 to 1.25 mm, buffer tube wall thicknesses of 0.05to 0.15 mm, the number of optical fibers in each buffer tube from 8 to24, the diameter of the optical fiber including the coating and coloringlayers from 0.21 to 0.25 mm, the overall number of optical fibers in thecable from 72 to 288, the number of buffer tubes in the cable from 6 to12, the central member minimum diameter, including the strength elementsand upjacketing (e.g., polymer coating on the strength elements,) from0.88 mm to 4.37 mm, the minimum cable core diameter from 3.22 mm and7.41 mm, the fiber density in the cable core from 3.49/mm² and17.64/mm², and the Ω parameter (fiber diameter/inside diameter of thebuffer tube) from 3.67 and 5.81. The examples herein show that thediameter ratio parameter Q ranges from 2.25+0.143(N)≤Ω≤1.14+0.313(N) andin some preferred embodiments ranges from 2.25+0.143(N)≤Ω≤2.66+0.134(N).

Low Attenuation Buffer Tubes/Cables with Small Particle Additive

In addition to the designs discussed above, Applicant has identifiedthat one source of bend related attenuation within a fiber opticcable/buffer tube is bending losses (e.g., microbending losses)associated with interaction between optical fibers and large sizedparticles (e.g., large water absorbing particles such as SAP particles).In conventional buffer tube cable designs, large sized particles, suchas SAP particles, (e.g., SAP particles having diameters greater than 50microns, greater than or equal to 75 microns, etc.) are thought to beadvantageous due to manufacturing advantages, such as ease of particlehandling during cable/buffer tube assembly, and due to commercialavailability of large sized particle material.

In contrast to conventional designs, Applicant has discovered thatutilization of small diameter particles in applications where contactbetween the particles and the optical fibers will occur significantlydecreases signal attenuation, e.g., during bending and/or thermalcycling. The improved signal attenuation performance provided by thesmall diameter particles discussed herein is even more significant whenused in conjunction with densely packed buffer tubes/cables as discussedherein. Specifically, in the case of densely packed buffer tube/cabledesigns discussed herein, the small diameter particles allow forsufficiently high particle quantities within the buffer tube/cable toprovide the desired particle functionality (e.g., waterabsorption/blocking of SAP particles, flame reduction in the case offlame retardant particles, etc.) without the particles undulyconstraining/impacting optical fibers during bending/thermal cyclingwhich would otherwise result in significant signal attenuation.

Referring to FIG. 15 , a buffer tube 100 including a plurality of smallactive particles, shown as small sized particles 102, is shown accordingto an exemplary embodiment. In the specific embodiment shown, buffertube 100 is substantially the same as densely packed buffer tube 22′discussed above. As used herein, active particles include particles offunctionally active materials, such as water absorbing materials,including super absorbing polymer particles (SAP), including particlesof sodium or potassium sodium acrylate or acrylamide copolymer, fireretardant materials, including magnesium hydroxide and aluminumtrihydrate particles, and smoke suppressant powders, includingmolybdenum based particles. Further, as used herein active particlesexclude inert or inactive particles, such as talc, PTFE and graphitepowders, etc. that have been or could be used for various purposes suchas slip agents in some cable designs.

Further, it should be understood that, the small active particlesdiscussed herein may be used in conjunction with any of the buffer tubeand cable embodiments discussed herein. In various embodiments, thesmall active particles discussed herein may be incorporated into buffertubes 22, 22″ and 22′″ discussed above and into cables 10, 60, 70, 80and 90 discussed above. In the case of ribbon cable 90, the small activeparticles discussed herein may be located in the central cavity ofbuffer tube 92 surrounding optical fiber ribbons 96, and in the case ofcables 10, 60, 70 and 80, the small active particles discussed hereinmay be located in the central cavity around the outer surfaces of thebuffer tubes instead of or in addition to also being located within thebuffer tubes.

Referring to FIG. 16 , a detailed view of densely packed central opticalfibers 20 of buffer tube 100 are shown with small diameter particle 102.In general, Applicant has discovered that the maximum outer dimension ofparticles 102, shown as dimension PD, that is permitted without causingsignificant particle-based attenuation is related to the size of thespaces between the adjacent optical fibers 20 within buffer tube 100. Ingeneral, Applicant has discovered that the interaction/contact betweenoptical fibers 20 and particles 102 that occurs during bending, thermalcycling, etc. increases signal attenuation (e.g., microbending losses)experienced by the optical fibers of buffer tube 100.

Thus, as can be seen from the geometry shown in FIG. 16 , as the opticalfiber diameter D2 increases, the size of spaces, such as central space104, increases, and thus, the maximum allowable PD increases as opticalfiber diameter increases. In addition, as optical fibers 20 become lessdensely packed within buffer tube 100 (e.g., in the case of buffer tubes22″ and 22′″ discussed above regarding FIGS. 2B and 2C), the size ofspaces, such as central space 104, increases, and thus, the maximumallowable PD increases as fiber packing density decreases. It should beunderstood, that while FIG. 16 shows particle 102 as spherically shaped,particles may be non-spherical in shape, and in such embodiments, PD isthe largest outer dimension of the non-spherical particle.

In various embodiments, particles 102 are sized such that the average ofthe maximum outer particle dimension, PD, of particles 102 is ≤50microns, specifically is ≤38 microns, and more specifically is ≤25microns. In some such embodiments, PD is also >1 micron and morespecifically >10 microns. Thus, by utilizing particles having a maximumPD≤50 microns, ≤38 microns or ≤25 microns, low microbend attenuation canbe achieved. Further, by utilizing particles having a PD that is atleast 1 micron or at least 10 micron, a sufficient level ofmanufacturability and ability to handle the particulate material duringmanufacturing is believed to be achievable.

In specific embodiments, the maximum PD of all particles 102 used withinbuffer tube 100 is between 1 micron and 50 microns (inclusive), 1 micronand 38 microns (inclusive), 1 micron and 25 microns (inclusive), 10microns and 50 microns (inclusive), 10 microns and 38 microns(inclusive), 10 microns and 25 microns (inclusive). In specificembodiments, the particles 102 used within a buffer tube 22 have a verylow number of particles falling outside of the PD ranges discussedabove. For example in specific embodiments, particles 102 are sized suchthat less than 50%, specifically less than 30%, specifically less than10% and more specifically less 1% of particles 102 within buffer tube 22have a PD greater than 50 microns, greater than 38 microns or greaterthan 25 microns. In addition, in specific embodiments, particles 102 aresized such that less than 50%, specifically less than 30%, specificallyless than 10% and more specifically less 1% of particles 102 withinbuffer tube 22 have a PD≤10 microns or ≤1 micron.

As can be seen in FIG. 16 , because the sizes of the spaces betweenfibers, such as central space 104, increases as the diameter of opticalfibers 20 increases, Applicant has discovered that the low attenuation,upper size limit of particles 102 is related to optical fiber diameter,D2. Thus, in various embodiments, average PD is less than 30% of D2,specifically less than 25% of D2, and more specifically less than 20% ofD2. In some embodiments, average PD is between 1% and 30% of D2,specifically between 1% and 25% of D2 and more specifically between 1%and 20% of D2. In even more specific embodiments, average PD is between10% and 30% of D2, specifically between 10% and 25% of D2 and morespecifically between 10% and 20% of D2. In specific embodiments, averagePD is between 14% and 18% of D2, and more specifically between 15% and17% of D2.

Similarly, in various embodiments, the PD of at least 50% of particles102 within buffer tube 100 is less than 30% of D2, specifically lessthan 25% of D2, and more specifically less than 20% of D2. In someembodiments, the PD of at least 50% of particles 102 within buffer tube100 is between 1% and 30% of D2, specifically between 1% and 25% of D2and more specifically between 1% and 20% of D2. In even more specificembodiments, the PD of at least 50% of particles 102 within buffer tube100 is between 10% and 30% of D2, specifically between 10% and 25% of D2and more specifically between 10% and 20% of D2. In specificembodiments, the PD of at least 50% of particles 102 within buffer tube100 is between 14% and 18% of D2, and more specifically between 15% and17% of D2.

In yet other various embodiments, the PD of at least 90% of particles102 within buffer tube 100 is less than 30% of D2, specifically lessthan 25% of D2, and more specifically less than 20% of D2. In someembodiments, the PD of at least 90% of particles 102 within buffer tube100 is between 1% and 30% of D2, specifically between 1% and 25% of D2and more specifically between 1% and 20% of D2. In even more specificembodiments, the PD of at least 90% of particles 102 within buffer tube100 is between 10% and 30% of D2, specifically between 10% and 25% of D2and more specifically between 10% and 20% of D2. In specificembodiments, the PD of at least 90% of particles 102 within buffer tube100 is between 14% and 18% of D2, and more specifically between 15% and17% of D2.

In specific embodiments, as noted above, buffer tube 100 is a smalldiameter buffer tube, such as buffer tube 22, 22′, 22″ and 22″, andoptical fibers 20 are small diameter, bend resistant optical fibers asdiscussed above. In some such embodiments, D2 is ≤210 microns and morespecifically is 208 microns, and in such embodiments, average PD is lessor equal to 32 microns, specifically is greater than 1 micron and lessor equal to 32 microns. In other embodiments, buffer tube 100 may be astandard buffer tube and optical fibers 20 may be standard sized opticalfibers having a diameter D2, of about 250 microns, in such embodiments,average PD is less than or equal to 39 microns, specifically is greaterthan 1 micron and less or equal to 39 microns.

In specific embodiments, buffer tube 100 is a polypropylene buffer tubehaving an outer diameter of 2.5 mm and an inner diameter D1 of 1.6 mmand includes 12 optical fibers 20 each having an outer diameter D2 of250 microns. In other specific embodiments, buffer tube 100 is apolypropylene buffer tube for a drop cable having an outer diameter of3.0 mm and an inner diameter D1 of 1.8 mm and includes 12 optical fibers20 each having an outer diameter D2 of 250 microns. In other specificembodiments, buffer tube 100 is a PBT buffer tube having an outerdiameter of 2.5 mm and an inner diameter D1 of 1.8 mm and includes 12optical fibers 20 each having an outer diameter D2 of 250 microns. Inother specific embodiments, buffer tube 100 is a PBT buffer tube for adrop cable having an outer diameter of 2.85 mm and an inner diameter D1of 2.05 mm and includes 12 optical fibers 20 each having an outerdiameter D2 of 250 microns. In other specific embodiments, buffer tube100 has an inner diameter D1 of 1.1 mm and includes 12 optical fibers 20each having an outer diameter D2 of 250 microns. In other specificembodiments, buffer tube 100 has an inner diameter D1 of 1.4 mm andincludes 24 optical fibers 20 each having an outer diameter D2 of 250microns. In other specific embodiments, buffer tube 100 has an innerdiameter D1 of 1.18 mm and includes 24 optical fibers 20 each having anouter diameter D2 of 208 microns. In all such embodiments, the buffertubes discussed herein include active particles, such as particles 102,having an average PD that is less than or equal to 39 microns,specifically is greater than 1 micron and less or equal to 39 microns.

Referring to FIGS. 17, 18A and 18B, the attenuation performance ofbuffer tube 100 (or cables including buffer tubes 100) and smalldiameter particles 102 are shown compared to various other cabledesigns. FIG. 17 shows attenuation change at 1625 nm as a function ofstrain for a 72 single-mode fiber 6 position cable, having differentsized SAP particles, gel or no particles. Results show that buffer tubesutilizing novel small active particles, SAP having an average PD of 25microns, has substantially improved attenuation compared to buffer tubeshaving standard SAP GR-111 powder (non-spherical particles havingaverage PD of 75 micron).

FIG. 18A shows attenuation change at 1310, 1550 and 1625 nm as afunction of thermal cycling for a 72 single-mode fiber 6 position cablewith buffer tubes having standard SAP GR-111 powder (non-sphericalparticles having average PD of 75 micron). As can be seen in FIG. 18A,during cycle 9 (-50 degrees C.), attenuation increase is observed. Incontrast, FIG. 18B shows the same thermal cycling test as FIG. 18A, bututilizing a 72 single-mode fiber 6 position cable with buffer tubeshaving the novel small active particles, SAP having an average PD of 25microns. As can be seen in FIG. 18B, by utilizing the SAP having anaverage PD of 25 micron, no significant attenuation is observed, evenduring cycle 9 (−50 degrees C.).

In addition to providing the low attenuation performance discussedabove, the small sized particles, particularly small sized SAPparticles, are believed to provide a variety of additional benefits tobuffer tube 100 (as compared to conventional buffer tubes utilizing 75micron SAP). Applicant has discovered that the small sized SAP particlesdiscussed herein have significantly higher water absorption and hashigher cohesion following water absorption than standard sized SAPparticles. Thus, in specific embodiments, because of the increasedabsorption and/or increased cohesion, the small sized SAP particlesdiscussed herein allow for formation of buffer tubes with very lowquantities of SAP. In specific embodiments, buffer tube 100 has lessthan 10 mg of SAP particles 102 per meter length of buffer tube,specifically less than 5 mg of SAP particles 102 per meter length ofbuffer tube, and more specifically less than 1 mg of SAP particles 102per meter length of buffer tube. In such embodiments, these low levelsof SAP particles 102 still provide sufficient levels of water blocking,such that liquid water (at room temperature of about 20-25° C.) and 1meter head height does not migrate more than 1 meter inside the buffertube in a 14 days period. The optical fiber cable water penetration testis as prescribed by IEC-60794-1-2-F5B. These low levels of SAP are incontrast to buffer tubes that utilize standard 75 micron SAP particlesthat typically has 10 mg/meter or more of 75 micron SAP.

In particular, Applicant has identified that smaller diameter SAPparticles absorb more water per gram of SAP powder as compared to SAPhaving larger particle sizes. Water absorption by SAP powder is testedby the following procedure: in a covered container to limit evaporation,deionized water is added to 100 mg of SAP powder to form a saturated gel(i.e., no visible liquid water) and held over a 1 hour period andweighed to determine the water absorbency in grams of H₂O per gram ofSAP. Table 6 below shows that SAP powder particles having an average PDof 25 microns (spherical particles having a diameter in the range of4-35 microns) absorb greater than or equal to 220 grams of water foreach gram of SAP particle material. The SAP powder particles having anaverage PD of 63 microns (spherical particles having a range of 16-70microns) absorb greater than or equal to 197 grams of water for eachgram of SAP particle material. The SAP powder particles having anaverage PD of 75 microns (spherical particles) absorb greater than orequal to 185 grams of water for each gram of SAP particle material. TheGR-111 SAP powder non-spherical particles having an average PD of 75microns (range of 22-148 microns) absorb 166 grams of water for eachgram of SAP particle material. This absorption amount is significantlyhigher than the larger SAP particle sizes shown in Table 6.

TABLE 6 SAP Particle Size/ Water Absorbency Shape (microns) (g of H₂O/gof SAP) 75—non-spherical (GR111) 166 75—spherical ≥185 63—spherical ≥19725—spherical ≥220

Further, Applicant has tested yield strength of the gel formed fromdifferent sized SAP particles following water absorption. The sampleswere run on a parallel plate Dynamic Mechanical Analyzer at 20° C. using25 mm serrated parallel plates. A dynamic strain sweep from 0.01 to 100%strain at an angular frequency of 10 Rad/sec. was utilized. The storagemodulus and stress were monitored. A plot of storage modulus vs. stresswas run. Yield stress analysis was determined from the data. High yieldstrength is indicative of high water absorption. As shown in Table 7below, the small sized SAP discussed herein have significantly higheryield strength, further demonstrating improved water absorption ascompared to the larger SAP particles standard in conventional buffertube designs.

TABLE 7 SAP Particle Size/ Yield Shape (microns) Stress (PA)75—non-spherical (GR111) 4-7 75—spherical Not tested 63—spherical 3725—spherical 44

Rollable Ribbon Designs

Referring generally to FIGS. 19-35 , various ribbon embodiments aredisclosed that are configured to allow the ribbon to be bent, curved orrolled from an unrolled position to a rolled or curved position. In suchembodiments, optical fibers are coupled to and supported by a ribbonbody. The ribbon body is formed from a material that is configured toallow the ribbon to be rolled and unrolled multiple times as may beneeded in various applications. In various embodiments, the ribbonembodiments discussed herein may utilize a ribbon matrix that completelyor partially surrounds the optical fibers when viewed in longitudinalcross-section such that multiple optical fibers are held together in theribbon structure. Generally, the ribbon body is formed from a material,such as a polymer material, that has an elasticity and/or thickness thatallows for the rollability of the ribbon. In some embodiments, theribbon body may be formed from a plurality of discrete sections orbridges spaced along the longitudinal axis of adjacent optical fibers.In other various embodiments, the ribbon body is contiguous bothlengthwise and widthwise over the optical fibers.

Referring to FIG. 19 , a rollable optical ribbon, such as optical fiberribbon 210, is shown according to an exemplary embodiment. Ribbon 210includes a ribbon body, shown as ribbon matrix 212, and also includes anarray 214 of a plurality of optical transmission elements, shown asoptical fibers 216. As noted above, optical fibers 216 may be any of thespecific optical fiber embodiments discussed herein. Optical fibers 216are coupled to and supported by the material of ribbon matrix 212. Inthe embodiment shown, ribbon 210 is shown in an unrolled or alignedposition, and in this position, array 214 is a parallel array of opticalfibers in which the central axes 218 of each fiber (i.e., the axis ofeach optical fiber 216 perpendicular to the cross-section shown in FIG.20 ) are substantially parallel to each other. In other embodiments, theoptical fibers may be arranged in non-parallel arrays within ribbon body212 (e.g., two by two arrays, staggered arrays, etc.).

In the embodiment shown, ribbon 210 includes a single linear array 214of optical fibers 216. In some other embodiments, ribbon 210 includesmultiple arrays 214 of optical fibers 216. In some embodiments, ribbon210 includes at least two linear arrays 214. In some other embodiments,ribbon 210 includes at least four linear arrays 214. In still otherembodiments, ribbon 210 includes of at least eight linear arrays 214. Inyet still other embodiments, ribbon 210 includes of at least 16 lineararrays 214. In some embodiments, each linear array 214 of ribbon 210 hasat least two optical fibers 216. In some other embodiments, each lineararray 214 of ribbon 210 has at least four optical fibers 216. In stillother embodiments, each linear array 214 of ribbon 210 has at least 8optical fibers 216. In yet still other embodiments, each linear array214 of ribbon 210 has at least 12 optical fibers 216.

In the embodiment shown, each optical fiber 216 includes a centralportion 220 that includes an optically transmitting optical core 222 anda cladding layer 224. Optical fibers 216 also each include a coatinglayer 226. Details of the core, cladding and coating of optical fibersproviding the high levels of bend insensitivity are discussed above.

Coating layer 226 surrounds both optical core 222 and cladding layer224. In particular, coating layer 226 has an inner surface that contactsand is bonded to the outer surface of cladding layer 224. Coating layer226 also has an outer surface 228 that defines the outer or exteriorsurface of each optical fiber 216. In the embodiment shown, coatinglayer 226 is a single layer formed from a single material that providesprotection (e.g., protection from scratches, chips, etc.) to opticalfibers 216. In various embodiments, coating layer 226 may be a UVcurable acrylate material, and may have a thickness between 10 μm and100 μm. In the embodiment shown, an inner surface of ribbon matrix 212is bonded, adhered or coupled to outer surface 228 of each optical fiber216.

Ribbon matrix 212 is configured in various ways to allow ribbon 210 tobe reversibly moved from an unrolled or aligned position (shown in FIGS.19 and 20 ) to a curved or rolled position shown in FIG. 21 , whilestill providing sufficient support and structure for fibers 216. Itshould be understood that FIGS. 20 and 21 only show the end portions ofribbon 210 for convenience, as represented by the break lines shown inFIGS. 20 and 21 .

In the unrolled or aligned position, shown in FIGS. 19 and 20 , opticalfibers 216 of the linear array 214 are substantially aligned with eachother such that the central axes of the optical fiber 216 are parallelto each other and lie along the same central fiber plane 230. As usedherein, substantial alignment between optical fibers 216 allows for somedeviation between the central axes of the optical fibers and centralfiber plane 230, such that the central axis of each substantiallyaligned fiber is spaced less than 45 μm, in some embodiments less than20 μm, in other embodiments ≤10 μm, and in other embodiments ≤5 μm, fromcentral fiber plane 230 and/or the maximum vertical distance (in theorientation of FIGS. 19 and 20 ) between the center points of any of thefibers 216 is 90 μm or less. Further, in the unrolled or alignedposition, the horizontal distance (in the orientation of FIGS. 19 and 20) between the optical fibers 216 at opposing ends of array 214, shown asfirst end fiber 232 and second end fiber 234, is at a maximum permittedby the ribbon matrix structure.

To move from the unrolled position of FIG. 20 to the rolled positionshown in FIG. 21 , ribbon matrix 212 is bent or curved around ribbonlongitudinal axis 236. Thus, in the curved position, fibers 216 definean arc or curve around longitudinal axis 236, and the horizontaldistance between first end fiber 232 and second end fiber 234 isdecreased. In this arrangement, when rolled ribbon 210 is held straightthe central axes of optical fibers 216 are substantially parallel tolongitudinal axis 236. In the embodiment shown in FIG. 21 , ribbon 210in the curved position assumes a substantially circular arrangement suchthat first end fiber 232 is brought into close proximity or into contactwith second end fiber 234. In the embodiment shown, ribbon matrix 212 isconfigured such that when ribbon 210 is rolled, ribbon matrix 212 islocated on the inside of the rolled ribbon such that a surface 238 ofribbon matrix 212 opposite of optical fibers 216 faces longitudinal axis236. In specific embodiments, the rollable ribbons discussed herein maybe in a rolled configuration within the cable, and an end of the ribbonmay be returned to the unrolled position to be coupled to an opticalconnector, such as via use of mass splicing equipment.

In various specific embodiments, the structure and/or materialproperties of ribbon matrix 212 discussed herein provides for animproved ribbon that balances rollability with fiber support. In variousembodiments, ribbon matrix 212 only partially surrounds optical fibers216. In contrast to non-rollable conventional optical ribbons in whichthe ribbon matrix completely surrounds the optical fibers, it isbelieved the rollability of ribbon 210 is enhanced by providing a ribbonmatrix 212 that partially surrounds optical fibers 216. In thisarrangement, the partial surrounding of optical fibers 216 provided byribbon matrix 212 results in a ribbon 210 in which the outermost surfaceof ribbon 210 on one side of the ribbon (e.g., the upper side in theorientation of FIG. 20 ) is defined by surface 238 of ribbon matrix 212,and the outermost surface of ribbon 210 on the opposite side of theribbon (e.g., the lower side in the orientation of FIG. 20 ) is definedby outer surface 228 of optical fibers 216.

Further, in this arrangement, ribbon matrix 212 is substantially locatedonly on one side of ribbon 210. For example, as shown in FIG. 20 , atleast 90% of the material of ribbon matrix 212 is located on one side(e.g., above) of central fiber plane 230. In a specific embodiment, allor substantially all (e.g., greater than 99%) of ribbon matrix 212 islocated on one side of central fiber plane 230. In such embodiments,without ribbon matrix 212 extending downward between adjacent opticalfibers 216, optical fibers 216 are allowed to abut each other such thatouter surface 228 of each optical fiber 216 contacts the outer surface228 of at least one other optical fiber 216. As shown in FIG. 20 , eachof the interior optical fibers 216 abuts two adjacent optical fibers216.

Further, as shown in FIG. 19 , ribbon matrix 212 is a substantiallycontiguous ribbon matrix. In the embodiment shown, ribbon matrix 212 iscontiguous (e.g., an unbroken, integral unitary body with no gaps orholes) in the lengthwise direction for at least 10 cm, specifically forat least 50 cm and more specifically for at least 1 m. In a specificembodiment, ribbon matrix 212 is contiguous (e.g., an unbroken, integralunitary body with no gaps or holes) in the lengthwise direction for theentire length of the ribbon. In addition, ribbon matrix 212 iscontiguous in the widthwise direction such that ribbon matrix 212extends over at least two of the optical fibers 216. In the specificembodiment shown, ribbon matrix 212 is contiguous in the widthwisedirection such that ribbon matrix 212 extends over all of the opticalfibers 216 of ribbon 210. Applicant believes that this arrangementprovides suitable support and protection to optical fibers 216 whilealso providing a rollable ribbon 210.

Ribbon matrix 212 also has a thickness that provides a balance betweensuitable support and protection to optical fibers 216 and therollability of ribbon 210. As shown in FIG. 20 , ribbon matrix 212 has amaximum thickness shown as T2. In various embodiments, T2 is between 5μm and 150 μm. In other embodiments, T2 is ≤125 μm, is ≤100 μm, is ≤50μm, is ≤25 μm, and ≤10 μm. In some embodiments, T2 and the rangesdiscussed herein relate to an average thickness of ribbon matrix 212.

Ribbon matrix 212 is also formed from a material, e.g., a polymermaterial, such as a thermoplastic material or a curable polymermaterial, having a modulus of elasticity that provides a balance betweensuitable support and protection to optical fibers 216 and therollability of ribbon 210. In various embodiments, the modulus ofelasticity of the material of ribbon matrix 212 is ≤1500 MPa. In someembodiments, the modulus of elasticity of the material of ribbon matrix212 is greater than 1 MPa and ≤1500 MPa, specifically greater than 10MPa and ≤1500 MPa, and in some embodiments is greater than 85 MPa and≤1500 MPa.

In some embodiments, ribbon matrix 212 is formed from a single layer ofpolymer material having a modulus of elasticity greater than 10 MPa andless than 100 MPa. In other embodiments, ribbon matrix 212 is comprisedof two layers, an inner layer and an outer layer. In some embodiments,the inner layer is in contact with optical fibers 216 and the outerlayer defines the outer surface of the ribbon. In specific embodiments,the inner layer has a modulus of elasticity ≤1.5 MPa, and the outerlayer has a modulus of elasticity greater than 1000 MPa. In specificembodiments, the total thickness of the two layer ribbon matrix 212 is≤40 microns, and in other embodiments, is ≤30 microns, or is ≤20 micronsin still other embodiments.

In various embodiments, ribbon matrix 212 and optical fibers 216 may beconfigured to facilitate identification and connectorization of ribbon210. In such embodiments, ribbon matrix 212 and/or optical fibers 216may include coloring or printed indicia to identify the type, location,etc., of optical fibers 216 within ribbon 210.

Referring to FIG. 22 , another optical ribbon, shown as rollable opticalfiber ribbon 250, is shown according to an exemplary embodiment. Ribbon250 is substantially similar to ribbon 210 except as discussed herein.Ribbon 250 includes a ribbon body including a plurality of alternatingribbon bridges, shown as upper webs 252 and lower webs 254. In general,webs 252 and 254 are bands of polymer material that are coupled betweenouter surfaces 228 of adjacent optical fibers 216. In one embodiment,webs 252 and 254 are contiguous in the lengthwise direction and eachextends over at least two optical fibers 216. In another embodiments,webs 252 and 254 may be formed from a series of discrete webs separatedfrom each other in the lengthwise direction by gaps 255, shown viabroken lines in FIG. 22 . Whether continuous lengthwise or separated bygaps 255, webs 252 and 254 are spaced from central fiber plane 230 suchthat outermost, planar surfaces of webs 252 and 254 are substantiallyparallel to fiber plane 230 and are positioned tangentially to the outersurface 228 of adjacent fiber pairs.

In the embodiment shown, each web 252 and 254 extends over and iscoupled to two optical fibers 216. Webs 252 and 254 are positioned onalternating sides of ribbon 210 such that in the horizontal directionone web 254 is located between adjacent pairs of webs 252. Further, webs252 and 254 alternately define the uppermost and lowermost surfaces ofribbon 250 at the positions of webs 252 and 254. In this embodiment,webs 252 and 254 are relatively thin having a thickness between 5microns and 150 microns. Further, it is believed that the alternatingpositioning of webs 252 and 254 allows ribbon 250 to be rolled in eitherdirection, and by offsetting webs 252 and 254 from central fiber plane230, bending strain on the ribbon material may be reduced.

Referring to FIG. 23 , another optical ribbon, shown as rollable opticalfiber ribbon 260, is shown according to an exemplary embodiment. Ribbon260 is substantially similar to ribbon 210, except as discussed herein.Ribbon 260 includes a ribbon body including a plurality of ribbonbridges, shown as webs 262. In general, webs 262 are bands of polymermaterial that are coupled between outer surfaces 228 of adjacent opticalfibers 216. In some embodiments, webs 262 are contiguous in thelengthwise direction and each extends between the outer surfaces of twoadjacent optical fibers 216. In other embodiments, webs 262 are discretebridges separated from each other in the lengthwise direction by gapswithout web material and each extends between the outer surfaces of twoadjacent optical fibers 216. Webs 262 are spaced from central fiberplane 230 such that outermost, planar surfaces of webs 262 aresubstantially parallel to fiber plane 230, and webs 262 are locatedbelow the outermost portion of surface 228. In various embodiments, theangular positioning of webs 262 relative to the central fiber plan 230is shown by angle A. In various embodiments, angle A is greater than 0degrees and less than 90 degrees, specifically is between 5 degrees and45 degrees, and more specifically is between 10 degrees and 20 degrees.In a specific embodiment, angle A is about 15 degrees (e.g., 15 degreesplus or minus 1 degree). In various embodiments, webs 262 have athickness between 5 microns and 75 microns.

Referring to FIG. 24 , ribbon 260 is shown in the rolled or curvedposition according to an exemplary embodiment. In this embodiment,ribbon 260 is rolled such that webs 262 face outward from rolled ribbon260. Further, ribbon 260 is rolled defining an angle B between centerpoints of two adjacent optical fibers 216, as measured from a horizontalplane 264. In general angle B represents the degree of bend allowed bywebs 262. In various embodiments, angle B is between 10 degrees and 90degrees, specifically is between 15 degrees and 45 degrees and morespecifically is about 30 degrees (e.g., 30 degrees plus or minus 1degree). In an embodiment in which ribbon 260 includes 6 optical fibers216, webs 262 allow ribbon 260 to be rolled into a hexagonal array asshown in FIG. 24 .

Referring to FIG. 25 , ribbon 260 is shown in the rolled or curvedposition according to another exemplary embodiment. In this embodiment,ribbon 260 is rolled such that webs 262 face inward toward thelongitudinal axis of rolled ribbon 260. In various embodiments, webs 262may be formed from material having elasticity that allows ribbon 260 tobe rolled in both the configuration shown in FIG. 24 and in FIG. 25 .

Referring to FIG. 26 , another optical ribbon, shown as rollable opticalfiber ribbon 270, is shown according to an exemplary embodiment. Ribbon270 is substantially similar to ribbon 210 except as discussed herein.Ribbon 270 includes eight optical fibers 216 supported by ribbon matrix212. Ribbon 270 includes a plurality of strength elements, shown asaramid yarn strands 272, supported from ribbon matrix 212. In theembodiment shown, aramid yarn strands 272 are located in the center ofribbon 270 such that two end groups of optical fibers 216 are formed. Inother embodiments, aramid yarn strands 272 may be positioned at anyother positions within ribbon matrix 212. Further, in other embodiments,ribbon 270 may include other strength elements, such as steel wire,glass reinforced plastics, other strength yarn types, etc., in place ofaramid yarn strands 272.

Referring to FIG. 27 , another optical ribbon, shown as rollable opticalfiber ribbon 280, is shown according to an exemplary embodiment. Ribbon280 is substantially similar to ribbon 210 except as discussed herein.Ribbon 280 includes one or more regions, shown as regions 282, withinribbon matrix 212 that is formed from a different material than the restof ribbon matrix 212. In some such embodiments, regions 282 are formedfrom a polymer material having a lower modulus of elasticity than therest of ribbon matrix 212. Further, regions 282 may be formed from amaterial that has low bonding with the material forming the rest ofribbon matrix 212, and in yet other embodiments, regions 282 may bethinner than adjacent regions of ribbon matrix 212. In such embodiments,regions 282 act as separation points allowing groups of optical fibers216 to be separated from each other. In specific embodiments, regions282 are formed from a polymer material having a modulus of elasticitylower than that of the material forming the rest of ribbon matrix 212,and the modulus of elasticity of the material of regions 282 is between0.5 and 1000 MPa. In other embodiments, ribbon 280 may include othertear features, ripcords, scores, etc. in place of or in addition toregions 282. In specific embodiments, regions 282 may be coloreddifferently from the rest of ribbon matrix 212 or include printedindicia that provides an indication of the location of regions 282. Insome embodiments, regions 282 may extend the entire length of ribbon280, and in other embodiments, regions 282 may only be located atcertain portions along the length of ribbon 280 providing differingaccessibility to optical fibers 216, along the length of ribbon 280.

Referring to FIG. 28 , another optical ribbon, shown as rollable opticalfiber ribbon 290, is shown according to an exemplary embodiment. Ribbon290 is substantially similar to ribbon 270 except as discussed herein.In this embodiment, ribbon matrix 212 of ribbon 290 includes a region292 in which aramid yarn strands 272 are supported. In such embodiments,region 292 may be similar to regions 282 in that region 292 has a lowermodulus of elasticity than the rest of ribbon matrix 212, whichfacilitates separation of aramid yarn strands 272 from optical fibers216. Such separation of aramid yarn strands 272 may be desirable duringsome connectorization procedures.

FIGS. 29 and 30 show an optical fiber ribbon 300 in various curved orrolled configurations. It should be understood that optical fiber ribbon300 may be any of the optical fiber ribbon embodiments discussed herein.As shown in FIG. 29 , optical fiber ribbon 300 may be rolled into anon-circular curved shape in which optical fibers 216 surroundlongitudinal ribbon axis 236. As shown in FIG. 30 , optical fiber ribbon300 may be rolled into a spiral shape in which most of the opticalfibers 216 surround longitudinal ribbon axis 236 and the innermost endoptical fiber 216, resides at or near longitudinal ribbon axis 236. Insome embodiments, the rolled arrangements shown in FIGS. 29 and 30 , mayallow ribbon 300 to be stranded or otherwise located within a cablewithout first being located within a buffer tube. In such embodiments,the rolled structure of the ribbon provides an organization andappearance similar to that of a loose tube cable in which fibers arelocated within buffer tubes.

In various embodiments, when an optical fiber ribbon containing glassoptical fibers, such as ribbon 300, is rolled or folded into anon-planar array, the minimum bending stiffness tends to increasesignificantly because there will no longer exist a bend axis that allowsall of the glass fibers to occupy the neutral axis. As a result, notonly will the rolled ribbon be stiffer than a planar ribbon, but alsothe material of the ribbon body may also be subject to significant shearstress in order to maintain the rolled ribbon as a coherent compositestructure. In some embodiments, the material of the ribbon bodiesdiscussed herein have sufficient strength and elasticity to resist theforces associated with stranding of the rolled ribbon 300 into a cableand also those forces associated with the bending of the cable as it isstored, installed and put in use. In other embodiments, the ribbonbodies discussed herein are designed to intentionally separate at moremoderate stress levels, relieving stress as needed while remainingintact at sufficient intervals along the length to provide the intendedfiber organization benefit.

Referring to FIGS. 31 and 32 , the various ribbon embodiments discussedherein may be located within a polymeric buffer tube 310, which in turnmay be incorporated into a fiber optic cable. As shown in FIG. 31 ,optical fiber ribbon 270, which includes embedded aramid yarn strands272, may be rolled and located within buffer tube 310 without additionalloose strength elements. In another embodiment, as shown in FIG. 32 , anoptical fiber ribbon without embedded strength elements, such as opticalfiber ribbon 280, may be rolled and located within buffer tube 310, andadditional loose strength elements, shown as loose aramid yarn strands312, may be included within buffer tube 310. In other embodiments, therollable optical fiber ribbons discussed herein may be used withincables without buffer tubes surrounding the ribbons. In suchembodiments, the rolled optical fiber ribbons may be directly positionedwithin a cable jacket and may be stranded around a central strengthmember.

In various embodiments, the ribbon bodies discussed herein may be formedby applying a polymer material, such as a UV curable polymer material,around optical fibers 216 in the desired arrangement to form aparticular ribbon body. The polymer material is then cured forming theintegral, contiguous ribbon body while also coupling the ribbon body tothe optical fibers. In other embodiments, the ribbon bodies discussedherein may be formed from any suitable polymer material, includingthermoplastic materials and thermoset materials.

FIG. 33 shows an exemplary tool for forming a ribbon body. Tool 320consists of a block of abrasion resistant material bored with a seriesof fiber channels 322 to guide an array of optical fibers 216 that arepulled through tool 320. Resin channels 324 convey liquid resin in apath that intersects fiber channels 322 at the exit of the tool. UVcurable liquid resin as an example could be applied using the tool andimmediately cured by the use of UV lamps positioned at the tool exit toform the polymer ribbon bodies discussed herein. In various embodiments,the shape of the interface between fiber channels 322 and resin channels324 may be configured to form any of the ribbon body shapes discussedherein. Further, to form ribbons (such as ribbons 210, 260, 270, 280 and290) in which the ribbon body is only on one side of optical fibers 216,tool 320 would be operated to supply resin only through either the upperseries or through the lower series of resin channels 324. To form aribbon, such as ribbon 250 having ribbon body portions on both sides ofthe ribbon resin would be supplied through both the upper series andthrough the lower series of resin channels 324.

Referring to FIG. 34 , in various embodiments, any of the ribbonsdiscussed herein may be incorporated into a cable, such as cable 330.Cable 330 includes a polymeric cable jacket 332 and a elongate strengthmember 334 (e.g., a GRP rod, metal wire, etc.) located within cablejacket 332. A plurality of optical fiber ribbon containing buffer tubes310 surround strength member 334, and each buffer tube 310 includes anoptical fiber ribbon, such as ribbon 270 discussed above. It should beunderstood however that cable 330 may include any of the ribbonembodiments discussed herein in any combination. In various embodiments,a binding element, such as a helically wound binder yarn or thin filmbinder, may be located to the outside of buffer tubes 310 andsurrounding buffer tubes 310 and may act to hold buffer tubes 310 in astranded pattern (e.g., an SZ stranding pattern) around strength member334. In other embodiments, cable 330 includes no binding element.

In various embodiments, as shown in FIG. 35 , a cable 340 may includerolled ribbons located within the cable without buffer tubes 310. Insuch embodiments, the ribbons may be rolled and then stranded directlyaround strength member 334. In some such embodiments, cable 340 mayoptionally include a binding element surrounding the rolled ribbons, andthe binding element acts to bind the rolled ribbons to strength member334. In various embodiments, each rolled ribbon may be surrounded by abinder element that helps hold the rolled ribbon in the rolled position,and in some such embodiments, the binder element may be color-coded tohelp identify a particular ribbon within cable 330. In some otherembodiments, cable 340 may include one or more strength member (e.g., aGRP rod, metal wire, etc.) embedded within jacket 332 in place of or inaddition to strength member 334, and in some such embodiments, theoptical fiber ribbons are located within cable 340 without buffer tubes.

It should understood that the optical ribbons discussed herein caninclude various numbers of optical fibers 216. In various exemplaryembodiments, the optical ribbons discussed herein may include 2, 4, 6,8, 10, 12, 14, 16, 24 etc. optical fibers or transmission elements(e.g., optical fibers 216). While the ribbon embodiments discussedherein are shown having optical fibers 216 arranged in a substantiallyparallel, linear array, optical fibers 216 may be arranged in a squarearray, rectangular array, a staggered array, or any other spatialpattern that may be desirable for a particular application.

It is to be understood that the foregoing description is exemplary onlyand is intended to provide an overview for the understanding of thenature and character of the fibers which are defined by the claims. Theaccompanying drawings are included to provide a further understanding ofthe embodiments and are incorporated and constitute part of thisspecification. The drawings illustrate various features and embodimentswhich, together with their description, serve to explain the principalsand operation. It will become apparent to those skilled in the art thatvarious modifications to the embodiments as described herein can be madewithout departing from the spirit or scope of the appended claims.

While the specific cable embodiments discussed herein and shown in thefigures relate primarily to cables that have a substantially circularcross-sectional shape defining a substantially cylindrical internalbore, in other embodiments, the cables discussed herein may have anynumber of cross-section shapes. For example, in various embodiments,cable jacket 12 may have an oval, elliptical, square, rectangular,triangular or other cross-sectional shape. In such embodiments, thepassage or lumen of the cable may be the same shape or different shapethan the shape of cable jacket 12. In some embodiments, cable jacket 12may define more than one channel or passage. In such embodiments, themultiple channels may be of the same size and shape as each other or mayeach have different sizes or shapes.

Unless otherwise expressly stated, it is in no way intended that anymethod set forth herein be construed as requiring that its steps beperformed in a specific order. Accordingly, where a method claim doesnot actually recite an order to be followed by its steps or it is nototherwise specifically stated in the claims or descriptions that thesteps are to be limited to a specific order, it is in no way intendedthat any particular order be inferred. In addition, as used herein, thearticle “a” is intended to include one or more than one component orelement, and is not intended to be construed as meaning only one.

It will be apparent to those skilled in the art that variousmodifications and variations can be made without departing from thespirit or scope of the disclosed embodiments. Since modifications,combinations, sub-combinations and variations of the disclosedembodiments incorporating the spirit and substance of the embodimentsmay occur to persons skilled in the art, the disclosed embodimentsshould be construed to include everything within the scope of theappended claims and their equivalents.

What is claimed is:
 1. An optical fiber cable comprising: a plurality ofrollable optical fiber ribbons, each optical fiber ribbon comprising: aplurality of optical fibers, wherein each optical fiber comprises: acore; a cladding surrounding the core; at least one coating surroundingthe cladding such that the cladding is disposed between the core and theat least one coating; an outer diameter ≤210 microns as measured at anouter surface of the at least one coating; a mode field diameter of ≥9microns at 1310 nm; and a macrobend loss of ≤0.5 dB/turn at 1550 nm fora mandrel diameter of 15 mm; and a cable jacket surrounding theplurality of optical fiber ribbons defining an exterior surface of thecable and a cable core, wherein a core fiber density is greater than7.12 fibers per square millimeter as calculated by the total number ofoptical fibers divided by an area of the cable core as determined from aminimum cable core diameter.
 2. The optical fiber cable of claim 1,wherein the ribbon body comprises a plurality of discrete bridgeslocated between adjacent pairs of optical fibers, wherein each of thediscrete bridges are separated from each other in a longitudinaldirection by a gap.
 3. The optical fiber cable of claim 1, furthercomprising a binder element surrounding at least one of the plurality ofrollable optical fiber ribbons.
 4. The optical fiber cable of claim 3,wherein the binder element is color-coded.
 5. The optical fiber cable ofclaim 3, wherein the binder element is a thin film binder or a helicallywound binder yarn.
 6. The optical fiber cable of claim 1, furthercomprising embedded strength members embedded within the cable jacket.7. The optical fiber cable of claim 6, wherein the embedded strengthmembers are a GRP rod or metal wire.
 8. The optical fiber cable of claim1, further comprising: a plurality of small active particles located inthe cable core.
 9. The optical fiber cable of claim 8, wherein a maximumouter dimension of the small active particles is between 1 micron and 50microns.
 10. The optical fiber cable of claim 8, wherein the pluralityof small active particles are selected from the group of functionallyactive materials including water absorbing materials, sodium orpotassium sodium acrylate or acrylamide copolymer, fire retardantmaterials, and smoke suppressant powders.
 11. The optical fiber cable ofclaim 10, wherein the small active particles are water absorbingmaterials and include super absorbing polymer (SAP) particles.
 12. Theoptical fiber cable of claim 11, further comprising: a buffer tube,wherein the buffer tube has less than 10 mg of SAP particles meterlength of the buffer tube.
 13. The optical fiber cable of claim 1,wherein the at least one coating comprises a primary coating contactingand surrounding the cladding and a secondary coating contacting andsurrounding the primary coating and wherein the outer surface at whichthe outer diameter is measured is of the secondary coating.
 14. Theoptical fiber cable of claim 13, wherein the primary coating has adiameter of ≤165 microns.
 15. The optical fiber cable of claim 13,wherein the primary coating comprises a modulus of elasticity of ≤0.5MPa and a glass transition temperature of −25° C.to −35° C.
 16. Theoptical fiber cable claim 13, wherein the secondary coating comprises amodulus of elasticity of at least 1700 MPa and a puncture resistanceload of at least 25 g.